SCIENTIFIC ABSTRACT KUZNETSOV, A. A. - KUZNETSOV, A. A.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000928110011-8
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 20, 2000
• Sequence Number: 11
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

OOLORSHMK' I - S'; GMLZR, Z- I a LIMIr Ocnv. -,L..A-. , qlXAffAM, Jr. S.
Bffecttvaness of Using the
eflneries. nBakluskii operation' heat exchanger
In Petroleum r Aserb.neft.khos- 35 no.5127-28 mr 156.
(KLRA 9tlO)
(Heat exchangers) (Petro.leum--R~fining)

En=- SOV, Andrey Alekseyevich:. CHERVOVA, M.S., red.; SHEWSIONX0, TvA.,
(Now machinery and instruments] Novye mashiny i pribory. Lenin-
grad, Lenisdat, 1960. 58 p. (KMA 13:11)
1. Zamestitell prodeadatelys Leningredskogo eovuarkhoza (for
Kusnotsov).
(Machinery) (Instruments)

6TEPANENK09 B.N.~ otv. red.1 KOCHETKOV, N.K.,, red.1 KUDRYASHOY,
L.I.0 red.; KUZMSOVA A.A., red.; ROZENFELID, Ye.L.p
red.; VASIL , L.N., red.
[Chemistry and metabolism of carbohydrates; materials]
Khimiia i obmen uglevodov; materialy. Moskva, Nauka,
1965. 351 P. (MIRA 19:1)
1. Vsesoyuznaya konferentsiya po probleme "Khimiya i ob-
men uglevadov." 3d, 1963. 2. Institut khimii prirodnykh
soyedineniy U SM (for Kochetkov). 3. Institut biokhi-
mii Im. A.H.Bakha AN SSSR (for Stepanenko). 4. Institut
biologicheBkoy i meditsinskoy khimii AMN SSSR (for
Rozenfelld)~
41P"

KUZN-r.TSOY,_A.A.; SUDAKOV, Ye.N.
Horizontal alk7lation reactor decign. Xhim.i tekh.topl. i masel
10 no.1:40-45 A 165# (MIRA 18:4)
1. Groznenskiy ordena Trudovogo Krasnogo Znameni neftyanoy
institut.

GENADINNIK, I.S., kand.med.nauk; TANANYKIN, N.I.; KUZNETSOV, A.A.
Significance or one-stage multilayer tomosplenoportography in
the diagnosis of tumors of the organs of the spigastric region.
-Veot,rent.i rad. 40 no.500-34 S-0 165.
(MIRA 18:12)
1. Kafedra obahchey khlrurgii (zav. - dotBent P.M.Tarasov) i
kafedra rentgono-radiologii (zav. - dotsent A.G.Suntsov)
Chelyabinskogo meditainskogo instituta.

KOROTKOVO A.0.0 inzh.l inzh.
Using castingu from light nonferrous a2loys. Trakt. i
sellkhozmash. 33 no..10t4i-43 0.163. (MRA 17:1)
L Nauchno-issledovatellokiy inoti~ut tekhnologii traktor-
nogo i sellskokbozyaystvannogo mashinoatroyeniya.

S/874 62100010021019101V:
D21SX300
AUTHORS Aleynikov, A.L. and Kuznetsov A.A.
TITLE: Solution of the converse problem in the case of a
gravitational step
.SOURCE: Akademiya nault SSSR. Urallskiy filial. Institut goo-_
fiziki. Trudy. no. 2, 1962. Geofizicheskiy sbornik,
no, 3, 333-339
T Z) L-T This paper is concerned with the analysis of anoma-
lies in the gravitational acceleration with the view to obtaining
information about ~he presence and nature of semi-infinite prisms
below the surface. It is suggested that the position of the'upper
and lower faces of the prism (h and h,)) may be determined fron, the.
-ratio of- tho maximum values -6.flie horizontal gradient, V-k'~Xl an&- the
extremal value of -the anomaly.- -which -is given by (in.units of 11)
Vnax: h2
x 2 In (5)
4eax Ago dr(h2 hl)
Card 113
7 7
7-7: -.11 gj~"

S/871~
/62/000/002/,319/019
11olution of the,converse ... D218/1)308
where Ago 'is the value of the.anomaly at the point taker, as the
origin at which Vxz a Vnylzax. Fig. I shows a nomogr=,which may be
used to determine h -and h in units of H '(the mean depth of the
sur'iace).2Vie excess density can be datet
prism below the mined from
the Eormulas
+ (6)
2zl.-(h2'- hl)
VXnI2X
2k ln~L2
hl
where k is the gravitational constant. Examples of the applications
of this method to field observations are given. There ari-3 figures
and I table.
Card 2/3.,

KU7NXTSOV, A.A.
- - -------------- - -- -
Role of partial hydrogen pressure in the genesis of traps.
Dokl. AN SSSR 158 no.ltl23-125 5-0 164 (MIRA 17t8)
1. Nuuchno~luslcdovatelllskiy Institut geologill Ax~ktiki.
PredstavIcno akademikom V.S. Sobolev-ym.

VODOPIYANOV) V.1j.1 GADDRAlUiTMOV, I.Y-n.; KLIZIIETSOV, A.A.
Readerst r "ponse to the article by S.C. Dori senko, V.H.Ilubolltaev,
and P.IA.talushko, "Comparison of results of ntudying 3tresses
surrounding workings by means of photoelastioity and in nature";
"Ugollmt 196.1,, No.2. Ugoll 39 no.11:65 N 164.
(MIRA 18:2)
1. Pemskiy nauchnc~-issledovatellskiy ugoliryy ii)sU*.,ut. (for
Vodoplyanov, Gabdrakhimov). 2. Fermskiy politik-hr.J.ches'k-ly
institut (for Kuznetsov).

KMNETSOV9 A.A.
Comparison of factors affecting the cristallization of
effusive and intrusive traps. Dokl. AN SSSR 165 no.3:
66&-669 N 165. (MIRA 18:U)
1. Nauchno-issledovatel'Wdy institut geologii Arktiki.
Butimitted June 18, 1965.
Ni~

L It 206),,--,6 FWT((J)/Ly
,j.1 (~'L " (r. I;;T . . . . . .....
RZ AR, -Ap6oo535J URGE "CODE t---UR10413166100010OVID0941009li--
AUTHORSt Sobolev, A, Fe; Kuznetsov, A. A*; Yefremov, A. A.
ORG.- none ~4e I
J?
TITLEz Electronic integratoro Class 42, No,, 177646
SOURCE: Izobretoniya, promyshlonnyye obraztsy, tovarnyyo znaki, no& 1., 1966s 94
TOPIC TAGSa electronic circuits, pulse integrator
ABSTRACT: This Author Certificate presents an electronic continuous signal
integrator containing an integrating c,-.pacitor, To increase the integration
accuracy and the response rate., the signal is fed to the input of the pulse-amplitude
converter. The output signals are fed to the input of a pulse-width converter
at whose output the integrating storage capacitor is connected (see Fig* 1)9
Fig. 1. 1 - pulse-aiVlitude converterl
2
2 - pulae-vidth converter; 3 capacitor
Orig. art. has: 1 diagram*
SUB COM 091 SUHH DATEt 14ug64
Card 1/1 UDCt

KUZNETSOVI A,A,, inzh.
Use of fixmness values in the date'rminAtion of the unit resistance
of soil. Trakt. i sellkhozmash. 32 no.2:27-29 F 162. (MIRA 15:2)
1. Kuybyobevskiy seltakokhozyaystvennyy institut.
(soil physios)

KWITMOV, A. A.
"Zootechnical Bases for Covcrin~- NursinG Sovs." Cand AEr Sci,
KharIkov Zootechnicel Insty Min Agriculture USSR, KharIkov, 10,54.
(KL, ITo 9, Feb 55)
SO: Sun. Yo. (31, 26 Aug 55-Survey of Scien'Clific aml 'technical
Dissertations Defended at USSR 1-11igher Educational institutions
(14)
N

XuRETSOi, i. i.-
"Preventative Infed6iin of Idving Ampule-Packaged Oultures of laisbmania
tropics for the Purpose of Propbylaxis Against Spontaneous Infection With
Borovskiy Disease (Dermal laishmaniasis).80and Biol Soi, Turkmen Inst of
Epidemiology# Microbiology, and Hygiene,, Ashkhabad,, 10 Dec. 54. (TI., 30
Nov 54)
Survey of Scientific and Technical Dissertations Defended at USSR Higher
Educational Institutions (n)
SOs SLm. No. 521., 2 Jun 55

ROZIMMID, Y9.16.; SMIKA, A.I.;
Splittlag *f dextran by spleen wrtract. DoklJ3 UO 104 no.l:
113-117 3 155. (NM 9:2)
l.Laboratorlya fisl*l*gichookey Wail Akademil nauk SSM.
Prodstavlono skadmiken ToA.Ingeligardtam.

88046
S/139/60/000/006/010/032
E201/E491
AUTHOR: KuAnetsov.,-A.A.
TITLE; Dielectric Properties and Structure of Polycrystalline
Samples of the ZnO-TiO2 System
PERIODICAL: Izvestiya vysshikh uchebnykh zavedeniy, Fizika,
1960, No.61 PP-71-7
TEXT; On Professor G.I.S kanavi's recommendation, the author
investigated the permittivity and the loss-angle tangent of the
ZnO.-TiO2 system 08 a function of its composition and crystal
structure. Samples with the following molar compositions were
used!
lZnO- 9TiO2;
2ZnO- 3TiO2;
3ZnO- 2TiO2;
lZnO- 4TiO2-,
lZnO- 1T102,'
2ZnO- 1T102;
3ZnO- 7TiO2;
5.3ZnO- 4.7TiO2;
7ZnO- 3TiO2-
The samples were in the form of disks and plates. They were
prepared by pressing and subsequent firing in a Silit '.rnace
at 1250 to 1350*C using standard ceramic techniques.
Measurements were carried out at frequencies of 400 to 108 c/s
Card 1/ 4

88046
S/139/60/000/006/010/032
E201/Ek9l
Dielectric Properties and Structure of Polycrystalline Samples
of the ZnO-TiO2 System
and at 1010 t;/1,8 at temperaturea of 200 to 300*C.
At 3 x 10 to o Is and at 1010 c/s, measurements were carried
only at 200C. The following apparatus was uBed: an MLE-1 bridge
at audio frequencies, Q.-meters K18-1 (KV-.l) and ZYK .-I (UK-1) at
radio frequencies, a waveguide line 33- H (33-1) and an
instrument 36-t4 (36-1) at the highest frequencies. The
temperature coefficient of permittivity was measured with
apparatus THE-IM (TKYe-IM), The values of the permittivity
the loss-angle tangent (tan 6) and the temperature 2~oefficient of
permittivity (TKO of the nine samples are listed in Table I on
P-72; all these quantities were obtained at 5 Mels and 200C.
Fig.1 gives the concentration dependences of the permittivity and
tan 6 of the ZnO-riO2 system. The permittivity fell linearly
with increase of the ZnO content between 10 and 66.7 mol.% ZnO;
beginning from 66.7 mol.% ZnO, the permittivity rose sharply.
This rise was due to elastic electron1c and Ionic polarizations
as well as due to superimposed relaxation polarization. The loss-
Card 2/4

88046
S/139/6o/ooo/006/010/032
E201/E491
Dielectric Properties and Structure of Polycrystalline Samples
of the ZnO-TiO2 System
angle tangent rose linearly with increase of the ZnO content and
the rise became much more rapid at ZnO Concentrations greater
than 66.7 mol.%. Analysis of the Debye X-ray diffraction
patterns showed that in the ZnO-TiO2 system only one compound
(zinc orthotitanate, 2ZnO-TiO2) was formed; this compound had
spinel structure. Measurements of the frequency dependence of
c and tan 6 (Fig.2 to 4) showed that c was practically
constant within a wide range of frequencies (a small reduction
of e at low frequencies may have been due to relaxation
processes with long relaxation times). The loss-angle tangent
fell with increase of frequency and was low and frequency-
independent at lo5 to lo7 cls. The value of tan 6 did not rise
in the centimetre region. The temperature dependence of e and
tan 6 (Fig-5 to 7) indizated that the temperature coefficient of
-the permittivity of ZnO-TiO2 samples can be controlled by a
suitable selection of composition. It was concluded that some
of the ZnO-TiO2 materials may be used'in temperature-compensating
Card 3/4

88046
S/139/60/000/006/010/032
E201/E491
Dielectric Properties and Structure of Polycrystalline Samples
of the ZnO-TiO2 SYst6m
and stabilizing capacitors. There are 7 figures, I table and
18 references: 16 Soviet and 2 non-Soviet.
ASSOCIATION: Saratovskiy pedinstitut
(Saratov Pedagogical Institute)
SUBMITTED: December 31,
JL959
Card 4/14

84449
S/057/60/030/009/015/021
~1111r~ 11-4-311331) B019/BO54
AUTHOR: Kuznetsov, A. A.
- ----------
TITLE: The Character of the Frequency and Temperature Dependence
of & and tanS of Polyorystalline Samples in the System
Y1 Ln-O-- ~ 10 2 vj
PERIODICAL: Zhurnal tekhnicheskoy fiziki, 1960, Vol. 30, No. 9,
PP- 1087-1094
TEXT: The author studied the dependence of & and tan& on samples of the
system ZnO-TiO2 (Ref. 12), and in the present paper describes the
temperature dependence of these two parameters. The samples were composed
as follows: 1ZnO-1TiO 2, 5-3ZnO-4.7T '021 3ZnO-2T '02 , 2ZnO-1T '02 , and
7ZnO-3TiO 2* The mixtures of the two oxides were pressed into disks, and
then annealed at 1250 - 13500C. Table 1 indicates E, tanS , and the
temperature coefficient of the dielectric constan s of the five
compositions investigated, at a frequency of 5-10~ cycles and a
Card 1/3
-4,

84449
The Character of the Frequency and S/057/60/030/009/015/021
Temperature Dependence ofeand tani of B019/BO54
Polycryatalline Samples in the System
ZnO-TiO2
temperature of 201C. The diagrams of Figs. 1-4 show the dielectric
constants and the tangents of the loss angles as functions of the
frequencies. In this connection, it is particularly pointed out that
3ZnO-2TiO2 and 2ZnO-TiO2 show the same dependence. In the diagrams of
Figs, 5-8, these parameters are represented as temperature functions.
Table 2 indicates the volume resistivity of the samples. As can be seen,
the composition ].'ZnO-2TiO2 has the highest value, its structure belonging
to the spinel type. The author concludes from these results that the
augmented dielectric constant is not only conditioned by elastic electron-
and ion polarizations but also by superposed relaxation polarizations.
The spinel structure makes an increase in the dielectric constant
possible. It appeared to be possible to regulate the temperature
coefficient of the dielectric constant by varying the concentration. The
author supposes that the dielectric losses are caused by the motion of
weakly bound ions. An estimation of the activation energy of the ions
which participate in the conductance and in the relaxation processes
Card 2/3
'M

84449
The Character of the Frequency and S/057/60/030/009/Oi5/021
Temperature Dependence offand tan.4 of B019/BO54
Polycrystalline Samples in the System
ZnO-TiO2
yielded a value of about 0.1 ev. An electrochemical aging was not found
in investigations in the range between 150 and 2000C, which fact
convinced the author that the n-type conductivity was small in the
imples investigated. N. A. Bogoroditskiy and I. D. Fridberg (Ref. 1),
G. I. Skanavi and G. A Lipa eva (Ref. 2), Professor N. P. Bogoroditakiy,
Yu. M. Volokobinskiy e; al. fRef. 15), 1. Ye. Balygin and K. S. Porovekiy
(Ref. 16) are mentioned. There are 8 figures, 2 tables, and 18
references: 16 Soviet, 1 Japanese, and 1 US.
ASSOCIATION: Saratovskiy pedagogicheskiy institut (Saratov Pedagogical
Institute)
SUBMITTED. March 28, 1960

AUTHOR:
TITLE:
PERIODICAL;
s/196/62/000/018/009/017
E194/E155
Kuz;1atSoV-,__A_,A,.
Calculation of the permittivity of ceramic radio
dielectrics of the system ZnG-T'02
Referativnyy zhurnal, Elektrote khnika i energetika,
no.111, 1962, 9, abstract 18 B 45'. (In the collection:
"Materialy XXII Nauchn. konferentaii. Saratovsk. gos.
ped. in-t. Fak. yestestvozn*, fiz., matem., 19611,
('Materials of the 22nd Sc ientific Conference,
Saratov State Pedagogical Institute. Division of
Nntural Sci.ences, Physics, Mathematics, 1961'
Saratov, 1961,
TEXT: Ceramic specimens prepared by sintering mixtures Qf
oxides are a two-phase system consisting partly of zinc ortho-
titanate 2ZnO . Ti02,' which has a structure of the type of spinel,
and partly of rutile or zincite depending upon which of the oxides
was present in excess. If the mixture composition corresponds to
the simple formula 2Zno . Ti02 then a single-phase system is formed
consisting of Zn2 Ti04. A series of specimens was prepared in
Card 1/2

Calculation of the permittivity ... S/196/62/000/018/0()9/017
E194/E155
the system ZnO-TiO2 (the ZnO content ranged from 10 to 7001; mole)
and c of the specimen was calculated by the formula of
Likhtenekker and V.I. Odelevskiy on the basis of C components,
which were taken as follows; for ZnO 12, for TiO2 112, ajid for
Zn2TiO4 19. The measured and experimental values of e were
compared at a frequency of 5 Mc/s and a temperature of 20 OC;
for specimens containing UP to 505 mole ZnO agreement is good.
In the range of 50 - 70% mole ZnO the graph relating the meabured
e to the composition displays a clearly expressed minimum.
For a specimen of 70% mole ZnO the calculated value of c is low
by a factor of 1.5.
7 references.
Abstractor's notes Complete translationd
Card 2/2

K IUTLI XLTSUI V
Aids
"An Educational FIIA 'The Diode,'". A. A,
Kusnetsov) DW
78adlo" No TP p 64
Recambiy4s -use of a silent film on the diode,
intended for Intermediate schools, in radio
amateur clubs. technical schools, etc. Main
defect df~the film is that different types of
diodes produced by Soviet indutry vere not shown..
Similar films are needed for other radio equip-
ment.
_T84

XUZ "r, SDVj, K.
USMA019 - Television Receivers Oct 51
"Replacement of the Decoupling Bars in the KVN-49
Television Receiverp" A. Miznetsov
"Hadion No 10, pp 44, 41'
Suggests improved design of decoupling device for
UNA9 television receiver, which simplifies re-
placement of burned-out capacitors used for de-
coupling. In this methodp the chassis does not
have to be removed from the cabinet.
208T57

-1. =17~PRCVTMI'
A.
Dynamos
Electrostatic generator with belt conveyer. Elektrichestvo no. 1, 1952. Doktor Tekhn.
Nauk, Frof. Energeticheskiy Institut im. Krzhizhanovskogo AN SSSR.
SO: Mont List of Russian Accessions, Library of Congress, Arwril 195h uncl.

KUZNErSOV, A. 235T59
USSR/Electronics Radar Oct 52
Educational Films
"P Film on Radar," A. Kuznetsov
'Radio' No 10, p 59
The motion-picture industry has put out a nunber
of short.educational film on elec and radio
engineering subjects. 'This film on radar, pro-
duced by the Sverdlovsk Studio of Popular'Sci Films,
demonstrates the operating principles of radar.
Film illustrates the role played by radar in
World War II and its role today in sea and air
navigation.
235T59

KUZIMTSOV, A.
I "Now= ~
Conference on radialocation. Mor.flot.15 &o.11:30-31 1 155.
(Ra4a ) (MLRA 9:2)

KUZNL-ISOV,.A.A.; KAZANTSEV, V.A.
Work on the optional subject *Directing a radio club in a school.*
Politakhoobucb, n0,2:55-59 7 159# (MIRA 1213)
1. Pedagogichaskty institut, go Saratov.
(Radio clubs)

APRAWINj L.; KUZNETSOV9 A.; IUDOVICH,,,Tu..,,prepodavate1' fiziki (Moskva)
A radio engineering ibotitute helps the school. Radio no.12slO D
160o (MIRA 149-1)
1. Institut radiotekhnild i elektroniki AN SSSR.
(Badio--Zduoation and training)

KUZNETSOV, A.. starshina. 1 stat'i
Struggle in silence. Starsh.-serezh. no.12:13 D 161.
(MM 150)
le Komandir otdeleniya gidroakustikov, Tikhookeanckiy flot.
(Sonar)

vol-ymv--~, rc.-d.
(Elactronle distance measuring system wid, two Integrntonil
Slektrormyi daltz=mcr a d%wlu InLogr;.torant, t'.fi-Avap I -d-
Vo "~;OVOLskoo radio," 1964. 183 il--. (!!J11"t 18.1)

ACC'NRI ARG0105870 SOURCE -C
AUTHOR: KanWov, K.; Kuznetaov, A. A.; Vallyev, A. A.
_i- IT7~ ;/1
TITIX: On the Investigation of thermoelectric properties of ferromagnetto sen~dconductors
11121169
SOURCE: Ref. zh. Elektronika I yeye primenenlye, Abs &
REP SOURCEi Sb. aspirantak. rabot. Dagestansk. un-t. Yestestv. I fiz.--matem. D.
Makhachkala, 1964, 135-JL46
TOPIC TAGS: ferromagnetic material, nickel base alloy, zinc base alloy, semiconducting
material, thermal EMF, resistivity, f 4 e t- m o e (c c-+ t- %G P"Joef- +Y VI
ABSTRACT: Results of measurements of thermal emf and resistance P of nickel-zinc
ferromagnetic semiconductors of the NI(x)ZnO(y)FeZO3(50) type of various conipositl6in-,are
given. -An Investigation Is made of speolmens the composition, of which is determined by the
following values of x and K(In. mole %): x = 0-60, y = 50. -7.5. In the transition from a zinc
ferrite to a nickel ferrite, the values of c' Increase linearly by a factor of v 2 (the measurement
temperature is 3 K). In the region of 300--600 K, the Kelvin temperature a for all ferriteo,
except pure nickel forrites, to negative. The dependence a (T) for the majority of the speoi-
mens is weak. In the oasowhen individual forrites reach the region of magactla traxwforma-

,ACC NR, A116016870
tion a sharp change In the fluctuation of (T) Is observed, which Is related to the Increasing
participation of conductivity electrons in the transitory processes, and also In the change in
distances between atoms. The activation energy determined according to p (T) increases as
P increases and Is equal to 0.21-0.3 ev for different ferrites. . The mobility of the electrons
u = 1/ne P, where the electron concentration n Is estimated froma, Is equal to 10-4-10-3
cm2/v.sec. The effective mass of carriers Is estimated to be equal to 2-7, The mothodology
of the measurements Is described, Trwwlation of al)Btraot] V. K,
SUB.CODE: 09,20
Card 2/2

L 44784_66 E14T(d)/EWT(M)/EWP(w)/,EWP(vjp--_22BE'
__Z k) Ijp(c) EM'
____ Z
ACC NR, AP6030254' SOURCE CODE: -LiR/014T/66/000/003/0 T
AUMOR: Kuzneteov, A. A.
ORG: none
TITLE: Dependence between weight, drag and cost of a one-time aircraft
SOURCE: IVUZ. Aviatsionnaya tekhnika, no. 3, 1966, T6-84
TOPIC TAGS: aerodynamics, aerodynamic drag, cost estimate, aircraft performance
ABSTRACT: An economic criterion for evaluating the optimum construction design of an
aircraft is considered according tc; which the cost and performance of the aircraft
are compared. Two problems concerned with the' relationship between weight, drag, and
cost of a one-time, single-stage aircraft with a given tactical load (useful + equip-
ment weights) and an invariable predetermined flight program are solved. The first
consists in determining the variation of the weight and cost of every separate system
of the glider, engine, fuel, and the whole aircraft with changes in the tactical
weight, without taking into account the cost of tactical load. The second consists
in determining the variation of weight and cost with changes in the aerodynamic drag,
Formulas are derived for two coefficients C and C called "the equivalent cost of
G
weight" and "the equivalent cost of drag" respecz~vely, which may be used for
optimization of flight parameters in the process of designing an aircraft. Orig. art.
has: 58 formulas. [ABI
SUB CODE: 01/ SUBM DATE: 27Nov65/ ORIG REF: oo4/ oTH REF: OOl/ ATD PRESR! 5079
Card 1 /-1 UDC: 533.6.013.12

-L-16901-
ACC NR: AT6003576 DIA(l) SOURCE CODE: UR/0000/65/000/0-00/0257/028-2
~AUTHOR: Kuznetsoy, A. Ao
176;
ORG: None A- k
0 Aq
TITLE: Determination of, initial conditions In the launching Of 4 flying craft from a moving
platform
SOURCE - Issledovaniya po dinamike poleta (Research on flight dynamics), no. 1.
*oscow, Izd-vo Mashinoetroyentye, 1965, 257-282
TOPIC TAGS: missile launching, mobile missile site, missile trajectory, trajectory
determination
ABSTRACT: - The author notes that the flight of a craft (for example, a rocket or missile)
begins at the moment Its final support section leaves the guide rails of the launching ramp.
Normally, it to from this Instant on that there is a solution of the diffe. rent 41xquattons for
the motion of the center of gravity and of the differential equations for thAmztion about the
center of gravity in the determination of the trajectory parameters of the apparitus. The
solution of the equations requires a knowledge of the initial conditions; that is, the condi-
tions under. which the apparatus leaves the guide rails of the ramp. The compleotity of the. 7--
;,Card 1/2 UDC629.198.24.005-

L 16goi-66
ACC NR: AT6003576
determination of these initial conditions when the launch takes place from a moving platform,
(as in the case of a launch from a vessel at sea) derives from the fact that the vessel Is
subject to roll and has its own speed of movement, so that the guide rails will be arbitrarily
oriented with respect to the basic planes of the vessel. In addition, the apparatus may be
affected by wind of arbitrary direction. The present author makes use of a wide range of
constant and variable values to determine the initial conditions of Interest in such.cases.
It is assumed that the speed of the vessel as well as wind direction and velocity remain
constant while the craftitravels along the launch ramp guide rails. The relative speed of
emergence (the speed of the center of gravity of the craft with respect to the rails at the
moment the craft leaves the.railB), the absolute (course) speed of the craft at the same in-
stant, the air speed, the angular velocities of the craft when leaving the guide rails due to
the roll of the platform -bearing vessel, and several critical angular values which have a
decisive Influence on initial trajectory conditions are determined. Orig. art. has: 8
tables, 9 figures, and 109 formulas.
SUB CODE: 16/ SUBM DATE: 02Aug65 ORIG REP: 003 OTH REF: 001
Card 2/2,s7ff/

ACC NR, AP7002677- SOURCE -CODE i---UR/0109/671012/001/0150/0153
Mash, D.I.; Skuratova, NeVe
AUTHOR: Kuznetsov
ORG; none
TITLE: Effect of an axial magnetic field on-'the output power of a
neon-helium laser simultaneously generating-the 3,39 and 0,6328 P lines
SOURCE: Radiotekhnika i elaktronikat Y, 12, no, 19 19679 150-153
TOPIC TA GS: gas laser, laser energy, neon, helium, do"~_/U"TZ_0~ dqc'~t
-VYuS-v-k:-K._
ABS, ACT:
,The effects of an axial d-c magnetic field on the power output of helium-neon
,lasers operating at'A wq3Z8 and 33,900 A were examined. The laser used a
160-cm-long quartz tube (inside diameter, 8 min) filled with a helium-neon
e with
Imixture and termiftating in quartz windows placed'at the Brewster angl
respect to the tube axis. Excitation was eatablished with a high-frequency
'generator. The longitudinal d-c magnetic field was generated by four
I
,23-cm-long coils (18,900 turns in eagh coil). spaced regularly along the laser
tube. Output power of the X - 6328 A radiation was determined by measuring
the currePt. sienerated in a'n FSK-1 photocell. and the power of the X.- 33,900 Al
7
Card 1/2 UDCs 621.373.029.67.ool
F

ACC NRs AP7Oo26_77_
radiation was established with a PbS _d2tector. The dependence of the output
power on the pressure of the A - 6328 A radiation was found, and for each
-value of pressure the optimal pumping power was determined. The above
proEedure was repeated in the(presence.of a magnetic field; the pumpigg power
and -the coil current, for all pressures, were chosen 'to give maximum radiated
power for X - 6328 A. The maximum radiated power for X - 6328 X increased b
Y,
.a factor of 1.5 after the magnetic field was applied. The optimal pressure
'(for peak output power) in the presence of the magnetic field was somewhat
.greater than the pressure with no magnetic field, and the working pressure
range is somewhat greater in the presence of' the magnetic field. -Changes in
.output power caused by variations in the magnetic field were studied for both.
,wavelengths, and at optimal presilires for the*A - 6326 A radiation. The
output powel for A - 6328 A increases and then decre.asse, whereas,that for
A - 33,900 decreases as the magnetic field increases until oscillation
ceases.
SUB CODE: 20/ SUBH DATEs o6Hay66/ OTH REPt 003/ ATD PRESSt 5114

8/05Y60/030/05/14/014
B012 Bo56
1UTHORt Kuznetsov, 1. A,
TITLEt Mechanical Stresses in an Immobile and in a Rotating
Cylinder loaded With a Homogeneous Electric Current
PERIODICALt Zhurnal tekhnioheekoy fiziki, 1960, Vol. 30, No. 5,
pp. 589 - 591
TEXTt For the purpose of determining mechanical stresses in electric
lines, differential equations of the elasticity theory may be used. These
equations contain the electromagnetic force of volume. The electro-
magnetic force in the line may easily be represented by such a form of
equation. It is pointed out that this advantage has hitherto not been
utilized by anybody (Refs. I - 3), and that therefore also the elasticity
theory could not be applied. Here, the mechanical stresses in an immobile
and in a rotating cylinder loaded with a homogeneous current are
investigated by means of the equations of the elasticity theory in con-
sideration of the electromagnetic force of volume. The solution of the
problem is given. There are 4 referencest 2 Soviet and 2 English.
V'B
Card 1/2

Mechanical Stresses in an Immobile and in a
Rotating Cylinder Loaded With a Homogeneous
Electric Current
S/05 60/030/05/14/014
2012YI3056
ASSOCIATIONt Fizicheskiy institut. im. P. N. Lebedeva AN SSSR Moskva
(Physics Institute imeni P. N. Lebedev of the AS USSR,
Moscow)
SUBVITTEDs August 29, 1959
Card 2/2

IMNIIPSOV, A.A.
Xechanical stresses caused by a radial electromagnetic force In a
multilayer coil with a homogoneous current load and rectangular vinding.
Zhur. tekh. fiz. 30 40-5:592-597 Ny 16o. WU 13:8)
1. 7isichookiy institut In. P.NJebedeva, AN SSSR, Moskva.
(strain and stresses)

KUZNF-TSOV, A.A.
T--- -
Mechanical stresses in the loops of the central protion of a
single-layer plan"spiral eoi.I*e&usd,* -radial electro-
magnetic force. Zhur.tekh.fiz. 31 no.8:944-947 Ag 161.
(KM 14:8)
1. Fizicheskiy institut imeni P.N.Lebedeva, AN SSSR, Moskva,.
(Straiza and stresses) (Elobtric coil..

i v r a as A s 'a -
A [I jme T-2
in a tatEre pl.cact in, a can ElwaarL
system of two mirrorq Rigred, et el.. J. Appl. Ph7s., 1962,
'l, 2 763) ;nd purniped by a r. UVCh-4, 1A-M, An-" -.,f I I Y..
- . J r - - -. . I The
a i -n oow,, r v r- a-9 c i grI r o nrpa atire
RmI I
um

Eo ~
, " ~ r- 4~ If 11 11 1 -.
- ~ I I . . - I
- I . .. 4 1 . I I '- . - ~ - . 1. ~ .. - . i

VAN GAN-CHAN [Wang Kang-chlang]; VAN TSU-TSZEN [Wang TS'u-TSeng];
DIN DA-TSAO (Ting Ta-tB'aol; IVANOV# V.G.; KLADNITSKAYA, Te.N.;
KUZNS DIN-Tr; NIKITIN, A.V*; OTVINOVSKIYp S.Ze;
SOLOVI I MOIG
Creation of antiprotona in the interaction of Yr- -mesons with
nucleons. Zhureekapoi teor-fiz 38 no.3:1010-1011 (MIRA 13:7)
lo O"byedinennyy inatitut yadernykh isaledovanAy.
(Protons) (Mesons) (Nucleons)

,44-010
AUTHORS:
TITLE:
PERIODICAL:
83755
S/056160/038/004/048/048
B006/BO56
Van Gan-chan, Van Tau-tszenj Veksler2 V. I., Virvasov, ReM.,
Vrana, I., Din Da-te_a_o_,_1_',T_m Khi In, Kjadnitpkava, Ye. N.,
Kuznetjmy, A. A, ,M klhru.L A., Rg-uyen Din Ty, Nikitin, A. Vot
i J
Solov'Yev, M. I.
Production of a '~--Ilyperonly Negative n--Mesons With a
Momentum of 8.3 Bev/c
Zhurnal eksperimentallnoy i teoreticheskoy fizikip 1960,
Vol- 36, No- 4, PP. 1356 - 1359
TEXT: In the present "Letter to the Editor", the authors give a detailed
report on the case of a Z--production and decay discovered by them for
the first time among 40,000 bubble-chamber photographs. The chamber hap-
pened to be in a 13,700-0e magnetic field. The photograph concerned is
represented as well as the track scheme. The tracks are numbered, and
the individual stars are denoted as "point A, B, 0, ..". The exact data
of the tracks and stars, respectively, are given in tables (Table 1:
"Kinematics at point A111 Table 2: "Kinematics at point B"; Table 3;
Card 1/2 Yn
Pig

Production of a f--Hyperon by Negative
n_-Mesons With a Momentum of 8.3 Bev/0
83755
S/05Y60~038/004/048/048
B006 B 05
"Kinematics at point 0"1 and Table 4: "Kinematics at points 01 and V
The individual tracks are identified, and the charges and momenta (mea-
sured and calculated) of the particles, the kinetic and mass energies,
and the total energy are given. For the stare B and 0 also the energy
balance is given. For B, the following is considered to be the most
probable reaction: ~ + C 4 He4 + 4P + 3n + n + + n- + nn 0. For the
primary star (Tables 3 and 4 )2 the following reaction is assumed:
n- + C --.* f- + Ko + f0 + K_ 4. P + n++ n- + recoil nucleus. The lifetime
of the f--hyperon was calculated to be (1.18+0.07).10 -10 see. G.A. Tilinny
and S. Z. Otvinovskiy are mentioned. There are 2 figures, 4 tables, and
4 references: 3 Soviet and 1 US.
ASSOCIATION: Ob"yedinennyy institut yadernykh issledovaniy (Joint
Institute of Nuclear Research)
SUBMITTED: March 24, 1960
Card 2/2

I
Ad
v
S
2

. I al
H
l

0
. : d 0
A 4

`
.0
V
-1
3
;

1 .0 .0
-*.- 1 0
:! ~.. - -

:2 ig d51 d d
5t-
d 0
is
-,**

Sa 2;1
ff fl

VEKSLERp V.I. j VRAKA; I.; KIADNITSKAYA~ Ye.N. j -XUDMSOV+-1.A,.;- MIHUL, A.R. j
MIHULv U.K.; NGUYEN DINH TIT; FE24EV, V.N.'j SOlDVIEV, M.I..-, HWOOKIpT.;
bMW-,LING-YEN.
On strange particle production in jr-- 6 interaction. Dubna,
I2datel'skii otdel Obvedinemogo ifi-ta ladernykh issledovanii.. 1961.
9 V.
(No subJect beading)

C/026/ 61/017/005/001/006
FOSO/FO04
AU THOR: Wang, Kang-ch'ang (3769/3227/2490); Wang, Chu-hsiang (3769/
4376/5046); Viryasov, N. M.; Ting, Ta-chao~(OOOZ/1129/6856);
Kim, Hi-in (6855/5593/0088); Kladnitskaya, Ye. N., Kutnetsov.
~,A ~Mikhul A.; Nguyen, Din-ti (708S/0002/6337); -Nikitin, A-.
and Solov';ev. M. L
-237 hyperons ~y the use of Z- mesons with a, mornew-
TITLE: Production.of :, -
tum of 7000 Mev/ c and 8000 Mev/ c
PERIODICAL: Wu Li Hatleh Pao, v. .17, no. 5, 1961, 205-213
TEXT: The productive cross section C(Cw 3.6 +_ 2 ItSiN at 6800 Mev/c.,
+ 4.4 +
6 ~USIN at 8000 Mev/c), mass M,- (Mv- a 1317.0 Z.Z Mev), and lifetime
10- - 3.2 0 %J ' -
t 5 13.4 x 10-1086c) of S-hyperson were determined by the use of Z mesons
~-TO(70 1~ 3. 1.Z Icand8OOOMev1c* In early investigations'! -hy~erons
~.having momentums of 6800 MOW
--C
4-
4'
-g5g R -57
~7'
R

C/ 02 6/ 61/ 017/005/001/006
Production of 'CA- hyperons by ... F050/FO04
were found by e)4eriments with cosmic rays. A butane bubble chamber 24 liters in
volume in a permanent magnotic field of 13700 gauss was used. The chamber was ir.
a-df
Mev/c and 8000 Mev/c-of lCmesons*_ A. three -dimensions amplifier and projectorwere
used to trace the negatives twice and sorrile negatives were traced three times* In the
tracing process those events which could be classified with S'hyperon decay-scherne
A VO + B, VO 4,Z + D, by appearance -were selected. The following standards were
applied In the determination oVE hyperons: (1) r must coincide with kinematics of-th
C-Aecay scheme Ao--+P + TC. (2) The refraction point must be within the AO decay plan.46
The vertical momentum of 7C meson and proton p, which came -from Ao decay relative7.
-,to the projecting direction of Ao, must be in equilibrium. (-3) The /\~ decay particles
o n the
should lie on the -.fracti nLpoi t
_plane formed by particles A and B. (4) At the r,
- ___ - _: OY
;vertical momentum of particles n) and B particle must be in equilibrium# 6 a-
-vents must satisfy kinematics of '-"hyperon decay scheme
ID + 65 bev
A + X
Card 214

C/026/ 61/ 017/005/001/006
Production of hyperons by F050/FO04
Among all the events there were U events which satisfied all 5 standards, Three events
coincided well.with the,kinematics of '- decay and have been claseffied with"
CA -,, hyperon.
Of all 21'_ hyperons, one wa's obtained by the bundle of Ir' mesons with 6800 Mev/c and
then were obtained by the bundle of IC' mesons with 8000 Mev/c. The results of this ex-
periment are listed in four, tables: (1) Table 1 lists data of defined,:'- . All these data
were average values which were obtained by using a microscope to measure two -four
times independently, It also lists the decay energy Q and lifetime of all Z"_ hyperons
found in their own coordinate systerno (2) Table 2 lists all.data concerning the primary
stars. These stars- have been analyzed as the source of ~-- hyperons. (3) Table 3 lists
the momentum p* in a TC- N mass center system, verticaT momenturn'p-l- , and projecting
L_J L_J_ hyperons were produced by the impact of Z- mesons
angle &* of S' hyperons (suppose
to free nuclei). The average vertical momentum (p~'_- ) of Z_ hyperon is equal to 318
35 Bev. This value is approximate to the vertical. momentum of proton and A hyperon.
This table also li'sts the characteristics of the following angles: (a) ti-* is the projecting
A
rn
angle of Ao which is projected out roma, hyperon decay process under its equilibrium-
Card 3/4

C/026/6'./017/005/001/006
i Production of hyperons by F0501F004
! system. (b) is the projecting angle of p which was projected out from the decay
P
process in its equilibirum system. Cc) WE-A* is the intersection angle between23i and
/~O decay planes. In the distribution of &-* and W- no asymmetry was observed.
(4) Table 4 lists the events which seems to be Among these events, four were in
the s ama- plane-and- four teen-were-in-different-planes. Most-of these events -in -the- same -
plane were induced by 7C'IC mesons; the others in different plane event
a may have been~
induced by Tc+,-It- or K7 mersons. Thanks are extended to V. (Wei Ke Shih
Lai Erh), 1. V. (Chi Wei Lo), L. P. (Chi Lo Wei Yeh Fu), N. I*
(Pa Pu La Fe). K. V. (Chi Ho Lo Fu). and L. N. (ChU Lao Yeh Fu).. There
are 3 figures and 4 tables. The Englis h- language references read-as follows: C. Fra&'
zinetti and G, Morpurgo, Suppl. Nuovo Cim. 6 (1957). 565; Wo B. Fowler et al. NuoVo--
~Cim. 11 (1959). 428.
lf:'SUBMITTED: March 20.-1961.,
.Card 4/ 4
T'!i

r A
J
X
3/05~/61/040/(61012/047
3102/3202
All-MORS. T.k.l.v, T 1.
,ing &--s'an, Invenov. T. G, i4A!za, is-
-Elad" t.k
Kusnotmov. A. A., Sguyan Din Ty, Pikitino Solov'Yov,
TITM Prcduotion of Ao(lo) hyperon4 and Xo mesons In r-p Intorac-
tions with a P- meson momentum ct 6.6 -0.6 lov/a
PERIODICALi Zhurnal skoperimental'noy I tocrotichookoy fialki, 1- 40,
. 2. 1961, 464-474
TZXTj The A*(Z:; and Ko production In V-p collisioni has hith;rto been
studied onli for threshold moment% of (0-9 - 1.4) Day/ci Ito ex lain the
nucleon structure and the Interaction, studio* must be mad* at higher *nor.
g he tu&i*a deecrit4d were a"& 1e th a 24-liter prop- V4bble ch-
b!r and a constant magnetic flold'of 13.700 ot. Tat expericent Is doeartb4d
in Ref. 2 (Zh-&TYt 3-8. 426t 1960). Tht pictures were taken with a stores-
;hotocazora with -Runsaxplazoat' objectives (focal length 67 on). 7h9 pic.
tures were evaluated 2 or 3 times with stereo-nagnifiers and reprojeotors.
CgnL_i,4I
4,
J

pro4u4sion of ... 31 02/1202
In this caste offLO141116Y Via 91 and 9V.. At and X* particles wore, solsoled
according to rigorous rults. Altogiethor, 233 ove,nts conforming to theeii
:rttort:aw apses se,glietv ant emoze,ma of theeee
t :" aloservodt
V 11 a calculated by the to computer -Ureel". 7ho values ob.
,a,. I'I *!y1rickily corr21:411noonsideratlon of %ht o'bo:rvation prob-
a Ilitt r . and X do4sys In the hasbor volume an wall 6 fordo? and
9 pro4uotian). The number of events. 19 which 0. 2. A. or 6 h.,gd p--
Vole,x war. coseerweed bo.1d.o X* an4jor A partials* ago glyp I '&%1$ 1.
"he mean number of jh&rged particles accom;anAng 4 4 or X pr:duction
was &too X-d masons wart o'cotryoA among those charSod particles.
.The nairal particles recorded wore produced In the reaction*
R' +p-A' + + ax
+ + + an
+0ex
+ P +
X, Ad 0V + +,V
+P-P +/(* +.Y +fix
+P-X* +K* +N +AX
P,

S/C5 6.1% 110. O/C=10*
?rceucticn of ... 2102/3202
oly,XI _011) 0 3 it), alio the rtactlan3
(X'R~ - a (S). a W/0 - a to), 0 WKI - 0 M
2 (Y-K' -1 - a (V'K'j - i (I'-K*), ,- - p Z' ~X' K*
- (K,. 9) - a (Alk~ -;~ a OVK-) ~ a :* K' K'
were poselblq. rn he f*IIWn6, -. viacticna are referred to only t-,r
'h-09 Mr1rogs jhv crop& oec-lonm are ~;r (~,. 'ha tots'. oros.
sat-on. OfA (C ) and X produotion a.,% r700 ;roton% was found to U
2-0 0-35 v,IJ ftacw~t 0: &.1 corriteic-, includinC the ~~ admixture
an., %~'. f.-iC1.nC7 of :n %t1a C43f.
(yar ") . 0.8 ~ 0.25 zb, ~(?Z) . ..2 z C.3 b. R
.:J Z C.2. Momentum "! ancular dl.tribt-Ups erg illustrated 'r. sayers.
4!acratne. The neon, t.ansvertt no-monta of i~ and X particles, 383 1 )5 and
393 z 35 MST40o rea;vc44vely, were #;Ijaol vtthim the limits of m4asurame%..
arrors. on tro:: avt1isnat -,he tx;vrIMIn%%I
' PAST P"'S40"
7 K LAII X K
r 9 t,.
Indi 11 at: *halt at , ontrpts.a 30 .. X 9 psir produttion areas
g th 'a
a tic is It, h r an that of T X 'he ratio read*
Card'3/tA

production of ...
0.710.2.
.he authors only studied XcA~*, X*X And i*Z*, and obtained
It
.,tar the production thresho'li (0-96 ~(Ycxa) 1.1 mbj I- drops to
0. 1 Ob as 1.2 3vy, and increases aj;ain to 0.6 mb at 1.3 3#~- T'* ratio
~( .&4 #xptritentsly determined I* be 0.71 the thooratloa-.y
ob!ained value (statistical theory) a. T.5. Mean 2ultiplicity, of ohs.-Itj
7axticleas At 6.8 Boy, not only alranCt particles bus also obarl.d And un.
tharged'partialts ~trt produced. ;n %ke 4444 of Multiple pion
the =tan number of th&rjeA particles was 3. - and In s1rango-par.
ticlo production, 9. - 2.%-00. Plons ConstitA%s thie lain ;art *0 charged
particles. It can be concluded from the Onercy balance in a production
even- that 'he numUer if pierm product& ta6ether vith a strang* particle is
Iover than In the as*0of ordinary multiplo pion P.-vdua%'.on. This Is In

Production of ... A102 "W
sdrvvm#n% with 1b. ...t.r q( t%irt, pica* %A-
*At v4t~#t. P-Attt~n is 24~. O.S-O.'2
Ai~,vildkr anA The & portment4l
A",,A in 4j.4r..s, '., it.- my t:6 I the A
hy;#rOAP abc. A *tjo,d %*n1qA:j 1~, 6#r--t ~A ts:A-14 Uftctsoo S
(f,forv./n b4ck_ 1,5). This soy-tTj -4$ ais) ~bs.rv#d ta C, 'aK Ice.
pro4u-ItQn *,#.ti y4t'.j A gy,s 1'e.tz'Al A.%. the -gul-
pt 1, .44 V r.jr. ;. it.. .. at, M.'T PtOdUS04 %080%b*2
.1, 44 hyperens tho. 4 fvrv*r3 2(
At righ- o! n, IhI6 is less dispAct, Ty"s
IA . I% t 4 lp;?.As ar.4
tr:;Ag Ih to
IL .0 t ~I %-;4r% ~% Aqctsm
44 It $104 4A trA, hCh at:
I the I it I ".v
,A f:tt13 , :. t"".
p Ici r, 0 A a a S -part
Sultion car. 69 00,11fat#j from the treAswerso mosenta Th.
hors obtaln-l WO 12. U.1 thank D, jlCkn1A1P*,. X. A. U ;o-,
y Cb:U Ki trb.O.,.
C

L. X. B..yay" for h.)p m %no %A4 Ki-
Xnl "- for it vi. of the 3. G. Dirz.. onj
V. Bm:14kcr urv coratcr.#4 Tr.-rt or, ~ !Igurvz. 4 t.tlo.. and 9 ret.t.rc#61
4 Zovi,141cc sr.3 5 T.. 1- r.f.r-cos to
p.tl-TL.ft# r..j *0 fbIl-A. fief S. D 4.1h#r, Ant. Intern. Coat. 0.
Cill Er.,rgy Physito .1 COO. I.A-1. I')'.,. k-C (,, 0. M.oachen. W. tcvl*r.
V. R. Vr.cht. PAY.. 11- WC W
ASJOCIATION, Cb*vll'.A,AOYY 10511tUt 7k4vfAYkt- 1001-40vARlY (Joist 146tstut-
~f $.Clear h,#*&rch)
SWITTLOs O.Ftfah.r f. 1960
rig. '% neent'a distributions or 40 hyp.r.no in it.* 0. 4. 6.1 6) total
Zgehctrum, t) the% of backward (solid lino~ and iorvar4 (dashed Line) oattlad
. y,,r,,,9'
pli. 2. h ..,ful., lidtributlen in the c. a. @.I %uaber of O.Onts given 14
parentheses.

MENU
23719
S/057/61/031/006/003/019
B109/B207
40 0 0 /* 13
AUTHORt. Kuznetsov, A. A.
TITLE: Force-free magnetic field coils of infinite length
PERIODICAL: Zhurnal tekhnicheekoy fizikip v. 31, no. 6t 1961, 650-656
TEXTt The author presents a method of computing the mechanical stresses
in coils of infinite lengthp possessing axial and circular magnetic
fields. 1) Mechanical stresses in a coil: If a and b denote the outer
and.the inner radius of the coil, and the (variable) circular and
Jlr J2r
(constant) axial current density, V the transverse Poiseon ratio, the
following relations are obtained for radial mechanical sfress:
A G2 [a' Jn2 a (1 (1 - 2-) bt 1, (1 a2
-21n
X
VV, b 4
4atb'l In
X at_rt_ b In (8)
(3 - 21A) (0 - bt) 3 - 21A
Card 1/5

S/057/61/031/006/003/019
lForce-free magnetic field coils of infinite... B109/B207
for the peripheral stress:
jt a2 at In$ a- 4- (1 2F) X
at ra
n
2 In In
X bt In (I -+- 20 r
-Fr
In
2
-4-r (S 2p)(,t-bie)
4
211) FS
[bt (In 4- .(9)
3 21- T
and for Cr at r- b
t)b- 't
(I 2p) b1l In
1-21L-i-2 b
GI - bs
IL
bj Ut In
S-2P P
2 21& al - bt (10)
2
Card~2/5
P",

S/0 41,11110 31 /006/00 3/019
-Force-free magnetic field coils of infinite... B1 09/B207
J1a
From (10) it may be seen that (6t)b - 0 when a arctan where a
a 2c a
denotes the angle between the current-density vector for r ---~-a and the
coil axis (Table 1). 2) Force,free magnetic coil: If R Iisthe expanding
force, and R the compressing radial volume force, the conditions for the
2
vanishing of all mechanical stresses read R R 1 + R2 - 0 and Rr-R 2-R.
a r p
J2r
Since R1-0J, r Jir dr and R2-4n -r fJ2r rdr this condition is fulfilled if.
r b
rR
R 2 27% r2Rdr
2 Rd, R (a a,
2 2 Rdr
Card 3/5

23719
S/057/61/031/006/003/019
Force-free magnetic field coils of infinite... B109/B207
a . arctan Jlr
~2r (19)
r
(a angle between the resulting current-density vector and the coil
r
axis). R
a C1
R (20)
lim C
r b 211
(C V C2 - arbitrary constants). With a finite expansion of the coil, the
forces R and R are not only functions of r but 'also of z, so that the
1 2
above conditions are only approximately valid. There are A table and
3 references: 1 Soviet-bloc and 2 non-Soviet-bloc.
ASSOCIATION: FizicheBkiy Institut im. P. N. LebedeVa AN SSSR Moskva)
(Institute of Physics imeni P. N. Lebedev, A5 USSR, Moscow)
SUBMITTED:
June 271 1960
Card 4/5

Z_ N (--: TS 0 V,
22124
S/056/61/040/003/004/031
.1~ 6 9/~ B102[B202
AUTHORSs Wang Rang-ohlang, Wang Tolu-teengy Viryasov, N.H.p Ting
Ta-tslaop Kim Khi in, Kladnitakayat Ye*N*# Kuznetsov# A#A*#
Mikhul, A., Nguyen Din Ty, Nikitin, A.V., SolovIyev,
TITLEs Production of - - hyperons by ly- mesons with the
momenta 7 and 8 Bev/c
PERIODICALs Zhurnal, eksperimentaltnoy i teoreticheskoy fiziki,
ve 40, no- 3, 1961o, 734 - 740
TEXTt The authors present comprehensive material concerning the produe-
tion oft--hyperons by negative high-energy pions in a 24-1 ;ropane bubble
chamber which was in a constant field Of 13P700 oe. These experiments
have already been described in an earlier paper (ZhFTF, I-So 426, ig6o).
27#000 photographs were evaluated 2 - 3 times for pions with 6 08+0.6 Bev/0
and 75#000 for pions with z 8Bev/c, The authors chose those eve;ta which
corresponded to a decay of cascade particles according to the mode
Card 1

22124
S/05 61/0401003/0041031
Production of-'!'- hyperons by B102Y5202
A--~ V0+ B9 Vo--) C + D as well as all sIngly-pronged stars from the vertex
of which a V0 particle departed. Altogether, 90 events were chosen; they
were measured by means of VNM-21 (UIM-21) microscopesq and the reaults
were evaluated by means of an eleotronio computer of the type "Dral"; 11
events of a:' -decay 0",-4 1 0+IT-+65 Mev) were identified according to
rigorous cri-teria. The angular and momentum characteristics of the 'Aden-
tif ied Z- hyperone are given in Table 1 , The events nos. 171-218 and nos.
19-179 are schematically shown in Figs.1 and 2, respectively. The Table
gives the data concerning the decay energy Q and the lifetime (until the
decay) of the-"-- hyperons. The mean value of Q from the 11-l' decay
events was Q a 61o9 + 2,2Mev from which the hyperon mass M=-- -1317,0+2,2
Mev was calculated, The mean lifetime was V -(3-5+3.4) 10- 10 see. The
0 -1.2 *
mean free path of thell- mesons in E--hyperon formation in propane was
I - (2 .02+2 86 ) cm for a momentum of 6.8 Bev/c and I - (0.68+0 29) cm for
-0:84 -0:20
- 8Bev/c. Assuming that the _'17--hyperon production cross section in nu-

Production of hyperons by ...
22124
S/056J61/040/003/004/031
B102/B202
olei is - A2/3 6 - 3-6 +2 5&~b is obtained with 6.8 Bev/c and
6 10.6+4:4 -2:1 ,
-3 2tLb with -8 Bev/a. Table 2 gives data on the primary stars
with ---- hyperon produotion. Table 3 shows the momentum (p#), transverse
momentum (p*)p angle of departure (0*) of the various particles as well
I
as the angle between the decay planes (LOO). Table 4 presents data 8n
the "background"events (4 oomplanar and 4 noncomplanar ones) where V par-
ticles were identified as A particles. Finally, the authors thank V.I.
Veksler and I,V. Chuvilo for di6cussionj L.P. Zinov'yev, N.I. Pavlov,
K.V. Chekhlovt L.N. Belyayev and various teams of technicians for their
assistance. There are 3 figures, 4 tables,and 7 references: 5 Soviet-
bloo and 2 non-Soviet-bloo.
ASSOCIATIONt Ob*yedinannyy institut yadernykh issledovaniy
(Joint Institute of Nuclear Research)
SUBMITTEDs September 30P 1960
Card 3/14-,l

B11TYAKOV, V.A.)- VAN YUII-CfW [Wang Yung-chang); VIRYASOV, N.V.)*
DU YUAIII-TSAY (Du Yuan-caih KIM KHI IN KLADVITSKAYA,
Ye.N.; KUZNETSOV, A.A.; NGUYEN, DIN TY iNguyen Dinh Tul;
PENEVI'l' '; f
Ye.S.; SOLOVIYEV, M.I.
[Properties of -7 O-resons-produced together with strange
particles in J7"--p and JT -c-interactional Izuchenie
svoistv -7T 0-mezonov, rozhdaiushchikhoia so strannymi cha-
atituami v Or ::p i JT -a vzaimodaistviiakh. Dubna, Ob"-
edenonnyi in-t iadernykh isoledovanii, 1962. IC p.
(MIRA 16;10)
(Mesons)

WAN YUNG-CHANG; VEKSLER., V.I.; DU YUAN-CAI; KLADNITSKMA~ Ys.N.;
KUZNETSOV A*A ; NGUYFN DDH-TU; SOKOLOVA, Y%$.; SOLOMEVp
;*N.1 MIHULj A.; SMIRNOVA; L,A.( ranalator]; SARANTSEVAO
V.R.,, tekhn: red.
A study of-A Ko and Kolko pair production in ir -P interactions
at the 9 - -meaon momentum of 7-8 BeV/o, Dubnao Wodinerq i
In-t iaderTWkh issiodovanii, 1962. 15 p.
1. On leave from the Institute of Atomic Physics, Bucharest1for Mikul).
(No subject heading)

VAN YU-CHAN (Wang Y, -ch'ang]; VEKSLM, V.I.; DU YUAF I-TSAY-----
(Tu Yuan-tslai; KIADNITSKMA, Ye.N.;
MIXHUL, A.; 11GUYEY DIN TY; PEREV, V.N.; SOKOLOVA., Ye.S.;
SOLOVIYEV, M.I.; SARANTSEVA, V*R,v takhn, red,
[Generation of A Ko and KOKO pairs in Or -F Interactions at 07
-meson energies of 7-8 Bev/c.] Izuchenie rozhdeniia -4 K 0 1 FOKO
-par v 5r -P - vzaimodeistvi-iakh pri impullse S-1 --mezona 7-8 Bev/s.
Dubna.. Ob"edineraWi in-t iadernykh iseledoyanlip 1962 15 ~
iMIRL 1;-.6)
1. Inatitut Atom-nov fi2iki, Bukhareat-(for Mikhul).
(mesons) (Nuclear reactidas)

VEKSLER, V.I.; VWASOV, NALI V11,111A0 Lj- KIM, IM INj KLADNITSKAYA,
Ye.11,1- KU21ETSOV AVAO- NGUYEV DIN TY; SOLOVIYEV, M.I.;
KHOFMO 1 0; IMI-YANI; SARANTSEVA, V.R., takhn. red.
(Polarization of.A-1Wperons produced in ;77~--p-interac-
tions at an energy of 7-8 Bev]Izuchenie poliarizatsii -A
-giperonov pri rozhdanii v 57- -p-vzabi:odeistviiakh s ener-
giai 7-8 Bev. Dubnay Ob"edinennyi In-t iadernykh isal.2
1962. 23 p. (MIRA 15:10)
(Hyperona-Decay) (Masons-Decay) (Protons)

BELYAKOV, V.A.,- BOYADZHiyzv, A.v.,. VAN YuN-cHAN(Wang Yung-chlang);
VEKSLER, V.I.; VIRYASOV, N.M.j KIM 101I IN; KWNITSKAYA,
Ye.N.; PZNBTWV.,.-A.A..,- MALITSEV, VA; NGUYEN, DIN TY;
PENEV, V.N.; SOLOVIYEV, M.I.; ZRELOVA, N.N.., tekhn. red.
[Production of A (E 0)-hyperons and Ko-mesons in the inter-
7- 0)-
action of 7 Gev. J1 -mesons with carbon) Rozhden-4e A W
giperonov i KO-mezonov pri vzaimodeistvii Vr--mezonov a
energiei 7 Gev s uglerodom. Dubna, Ob"edinenrqi in-t iader-
nykh issledovanii, 1963. 18 p. (MIRA 17t2)

BELYAKOV, V.A.; VRI YU11-CHAll [Wang Yung chlang); VEKSLER, V.I.:
VIRYASOV, N.E.; VRA?lA, I.; DU YUIJI-TSAY [Tu 'Yuan tslai];
KIM KIII IN; KIADNITSKAYA, Ye.14.1- RNNETSOV A.
1-11OULj E. ; NGUYEN, DIN TYi PAT
SOKOLOVA, Ye.S.; SOLON"YEV, M.I.; 00EYOKLI, T.;
14~IKHUL, A.
[Production of A-lWperons and Ko-mesons in ST -p-
interactions at an energy Of 7-8 Bev] Issledovanie protses-
0-
sov rozlideniia A--giperonov i K mezonov v JT P- vzaimo-
deistviiakh pri energii 7-8 Bev. (n.p. n.d.] 26 P.
(mesons) (Hyperons) (MIRA 16:10)
ME RE

MELYAMV, V.A., WANG YUNG-CFAM VFMZR, V.I., VIMWOV, H.M.,
DIJ ID1214-SAI, KD1 III IN, )aA1.'ITSkA'(A, Ye. Y.,, =M,'MW. A.A- I-1- , A.
NGUYER DBIG TI, 1, PATEERA, V. ITENEV, GONOL&A, Ye. 3,, COLUI-01,- M.I.,
110H.UXL, T., and TSEN LIN-IAN
"The Investigation ofAllyperon ande-Meson Production iniZOand
Interactions at T-8 Gey"
report presented at the Intl. Conference on Mgh Energy Physics, Ceneva,
4-11 July 1962
Joint Institute for Nuclear %search
Laboratory of High Energies
_Y I
z

F ., j X7 lee,
771 Atr
xm
Tr-MYAMV, V.A., WtV1, y1r.0-MAN V.T., Vill"
Elm III Iri xjAPji1MKAYAp Ye. A A. 411M, A., Pul TI, TF-;O"
sOYDI.ft, Ye. S., GoLovikv, M. 1.
"Study of A K and Ki r. Fair ProiluctiOn ifW-P and 76 Interactions at the
7-8 ('10Y/C Momntual Jrf -jfc.ons"
report presented at the Intl. Conference o .n High Energy rhYdicsy Genevat
4-11 July 1962
Joint Infititute for Nuclest 11caearch
Laboratory of High Energy FhySiCB

3/05 6/62/04 3/00 3/013/063
B102/b 104
AUTHORS: Wan6 YunC-chan6, Veksler, V. I., Tu Uan-ls'ai,
Kladnitskaya, Ye. N., Kuznatoovt A Mikhul, A. ,
Nguyen Din Ty, Penev Sok'olova, Ye. S. SoloylyevIll. 1.
0_6
TITLE: Investigation of AKO and K K -pair production in n p inter-
actione with n-meson momentum of 7-8 Bev/c
PERIODICAL: Zhurnal)eksperimentallnoy i teoreticheskoy fiziki, v. 43,
no. 3(9 , 1962, 615-8~--,
0
+K
TEXT: P air production events, including 52 (A+Ko), 37 (K --0),'16 either
(A+K') or (0+K') and two (A+K'+Ko) were observed. amon*g 60,000 photoeraphs
made wi.th a 24-liter propane bubble chamber. The momentum and angular
+ 0
distributions of the n , A and X particles were determined. Also ihe
distribution of
12 (Et,(x)EK PA(X)PK MOW). K) + ff?AjKJ + M110"' MA(10 - MIC
Card 1/3 (P momenta)

0 S/056/62/043/003/013/063
Investication of AK and... B1021B104
was studied and the results obtained were confronted with the theoretical
curves (Monte Carlo method). Results: The mean Ko momentum from
,~K0pairs .-,As 702 1 54 Mev/c, from KOP pairs 604.1 55 Mev/c. In the
Tc p c.r... In (55 t 9)% of the events the A particles from AKO pairs flew
back--.-~d and those from the Ko forward. In (33 1 7)%-they both flew
b,-..-'-,vard. In (12 1 4)~ they both flew forward or the A forxa'rd ana the
z' backward (this distribution indicates a contribution of peripheral
interaction). The A-hyperon distriVuton has a peak at -14 cosQ 4 -0. 8.'
A
For the KOO pairs a maximum in the Kodistribution was observed at
+0.6