SCIENTIFIC ABSTRACT FILIMONOV, P.V. - FILIMONOV, V.A.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000413030008-2
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 13, 2000
• Sequence Number: 8
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

BRiSKMY LoOnAd Yakolrlevich,- FILIMONOV, F.V., nauoInVy red.; CFISWV,
M.M., red.j BARAWYM-N.Ir'. ------- f~AE.-itd-; DORODNOVA, L.A..
tekhn, red.
[Safety measure3 for electric work in construction]Elektro-
bazopasnost' na stroitellstve. Moskvit, Proftek-bizdat, 1962.
115 P- (MIIL4 1!5: 8)
(Electric engineering-Safety measures)

FILIMDNOV, P.,V.
Ins-I.allation of unshielded 380/220 v. powor distribution boards
wit1i exposed current conducting parts. EnergetJk 10 no.4:34
Ap 162. (KRA 15:4)
(Electric power distribution-Safety regulations)
-5,
F7
-R, T
A,

FILIMONOV, F.V.
'A"MMUMMMMMM~
Electrical wiring in"explosion-hazardous system. From.
energ. 18 no.5:62 My 163. (~M 16:6)
(Electric wiring-Safety regulations)

SIIEVCHENKO, N.F.; FILIMONOV, P.V-
Electronic ENP and EXR automatic d.c. bridges. Prom, energ. 20
no.1:52-53 Ja 165a (MIRA 1894)

SHEVCHENKOS
SLI;VZG-114 signal lamp device. Prom. energ. 20 no.2:58 165-
Standardized uF-PK-VZG electric drive. Ibid.:59 (KIRA 18:4)

-,F-I.LIYC,IIOVP S.A.
The TUK-3 ultrasonic resonance thickness meter. Biul.takh.-ekcn.inform.
Gos.nauch.-iasl.inst.nauchj tekh.inform. 17 no.102-54 164.
(MA 17:2)

L;>48;)P-66-
W - , I~rP (C) ( N ) WIRil
AP6006955 SOURCE CODEs UR/0381/65/000/006/0061/0068
AUTHORS: -j~Ageg Yue V,; Filimonov, S. A.t Shishkina, N, V,; Pakhomov, Ve V.-
Veremeyenko, S. V.; yrkoii;~!'~--16z;--
ORG: none
TITLE-t UVFD-1 defectosco2g for controlling.multilayerecl,structurais and nonmetallic
parta
SOURCE: Defektoakepiya# ao. 6j, 1965# 6148
TOPIC TAGS: defectoscope, diagnostic instrument, electric device, electronic
circuit /UVI-M-1 defectoncove
ABSTRACT: The block diagram and detailed electric circuitry of a UVFD-1 defecto-
scope are given. fleforring to Fig. lp
&
Fig. 1. Block diallram of' a UWD-1
defectoaci3pe.
I ====21
Card 1/2 UDCi 620,179, 5

L 24822-66
ACC NRt Ap6oc 0
6955

the defectoscope consists oft I metal-lie base, 2 nonmatallic film depositj
3 - emitting oacinttor) 1, - receiving oscillator, 5 gent3rator to food power
to the vibrator# 6 - ampllflor, 7 - shaper, 8 - phase-measuring circuit, 9 - phase
regulator, 10 - shalvr, 11 - needle indicator, .12 - relay instrument, 13 - detector
for automatic regulitting
., of amplifications, 14 - amplitude ineasuring devico, and
15 - indicator. The instrument has four types of scanner heads that operate on a
frequency range 25-;.60 keycle, A sketch is included for one such scanner head
connected to the intstr=ent by a coaxial cable, The instrument weighs U kg and
is portable, It is used In conjuction with automatic recorders and is very useful
for controlling nomnotallic film deposits on metallic bases and for identifying
defects between the jointAi of milt1layor structures. Orig. art. has, 4 figures.
SUB CODEs
09/ SUBH DATEs 26Jun65/ ORIG REP: 005

Card 2/2
I 773.1-s- -r
Y

FILIMMOV, S.I.; IIIANOVA, L.N.
Apparatus for simultaneous registration of blood pressure and
sounds-within the heart. Trudy NIIEKHAI no.5-.241-244 161.
(MIRA 15:8)
1. Nauchno-issledovatellskiy institut eksperimentallnoy khirurgi-
cheskoy apparatury i instrumentov.
(BLOOD PRESSURE) (HEART-SOUNDS)

FILIMONOV, B.I.
Apparatus for gastric irrigation. Voen.-med. zhur no-5:80-81 W 157.
(MIG&TION, (" 12;7)
stomach, appar. (Rue))
(STOMACH,
irrigation, appar (Ras))

.-FILIMONOV, S.I., RbSTOVTSIV, B.N.
Improved apparatus for cardiac examination. Medeprom. 12 no.8246-47
Ag'58 (MIU 11:9)
1. Naiwhno-issledovatellskiy, inotitut eksperimentallnoy khirargicheak07
apparabtry i instrumentov.
~(HMART-JMAHIRATIOW)
(PETSIOLOGICAL APPARATUS)

Card 112 P
ub. 22 9/52
Authors A:.Oseyevskiy, N. E.; Prudkovskiv, G. I,.; I(ooo-til-ov, G. 1. and
Title
IMP10"""dr a fio-tI2,~nirorlli Magnetic field for the ptirpose of increas!",r;
the resoolving power of a mass-spectrometer
F,erlodical I D,)k,. AN 100/2,' 229-232, Jan 11, 1955
Abstract Lkperiwints conducted with mass-spectrometers are described. Thp,
pur- ose of the experiments was t-) find out the effect of a non-
uniform marnctic field used with the jiviss 3pectrometers on Lho
ressolving power of the latter. The results of tile experli-on1u;7,
3hoa thELt a non-uniform magnetic field increases the. ressolvint"
pIower of a mai3s-spectro:,teter by a factor of I
1 - n
Institution : Acad. of Scs of the USIR) S. 1. Varilov, InstItute of Physical
Problems.
Presented by : P,cadenticiar A. P. Alexandroff, E~eptembcr 30, 1954

DoIc. AN S""M 10012-, 229-232, Jail 11, 054
Card 2/2 Pub. 22 - 9/52
Abstract Where 71 lo- the coefficient of non-uniformity of the field.
It can be calcullted by the following formula:
S
dr 0 a,
JIL
iv the angle between gunernUce.,; of the magnetic conical Ups
uped for. the foinnation of Lhe non-uniform field. lo is the
width of the slit on the radioun, ro. Nine rof'r.-mices: I U,',,U;
2 German; 6 USA (1941-1952). Diagr~,uns; ginph,~.

Molt,"tl I
U
six -
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9,
uso cc D. .4
14' 0 ;1 a
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f 1.1: Id
w all
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9 ov ils S3,
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me
Hal
me
is ho
w ol a

KAPITSA, P.L.0 akadenikl FJLIMDNOV S.I.; KAPITSA, S.P.
Ti-aory of elect-ronin processes in a magnetron generator with
contlnuouti pawer output. Elektron. bolsh. moshch. no.3-.
7-35 164. (MIRA 17-,9)
1. Otvetsvennyy redaktor zhurnala "Elektronika bollsh-4kh
moshchanostey" (for P.L. Kapitsa).

FILIKONOV, S.I., inxho; GUZ=o Nol.9 isgronow-vinogradarl; red.;
PIMAII To... takhn.red.
Nechanization of grape murserlss3 Nekhanizateiia rabot v Tim-
gradnom pitowaike. lishinev, Goo.izd-vo "Kartia Moldovenlaake,*
1960. '131 p. (MM 14:3)
(Titiculture) (Agricultural =chinory)

DIBNER, Ye.E., red.; I,ISTENGUBT, M.A., St. nauchn- sotr. kand. sel 1 khoz.nauk, red.;
K?,YSAKHCIVICH9 Ya.A., kand. sellkhoz. nauk, red.; TARASOVA, A.YU.t
red.; FI:LIMONOII-., S I red.; SHKORUPEYEV, I.S., red.; SHLYAKHOVOY,
--=. . Y
YeAri .; SININA, V., red.; POLONSKIY, S., teklui. red.
[Mechanization of work in plant protection ]Mekhanizatsiia rabot Po
zashchite rastonii; sbornik trudov. Kishinev, Izd-vo selikhoz.
lit-ry, 1961. 187 P. (RRA 16.- 2)
1. Nauchno-teklinicheskoye soveshchaniye po voprosam konstruirova-
niya maiihin dlya zashchity plodovykh kulltur i vinograda. Kishinev,
1960. 2,, Predsodatell Moldavskogo respublikanskogo pravleniya
Nauchno.-tekhnichoskogo obshchestva mashinostroitellnoy promyshlen-
nosti, Izamestitell predsedatelya sovnarkhoza Moldavskoy SSR (for
Shkoruptyev). 3. Vaesoyuznyy nauchno-issledovatellskiy institut za-
shchity rasteniy (fnr Meysakhovich). 4. Moldavskaya stantsiya za
shchity rastenly (for Listengurt). 5. Zamestitell nachalinika G(-
sudarst-wennogo spetsiallnogo konstruktorskogo byuro po mashinam
dlya me'khanizataii rabot v sadakh i na vinogradnikakh (for Dibner).
6. Nacballnik :Laboratorii ispy-taniy mashin Gosudarstvennogo spe-
t3ialln,3go konstruktorskogo byuro po mashinam dlya mekhanizataii
rabot v sadakh i na vinogradnikakh (for Shlyakhovoy). Nachallnik
issledovatel'skogo otdela Gosudarstvennogo spetsiallnogo konstruk-
torskog,,o byuro po maehinam dlya mekhanizatsii rabot v sadakh i na
vinogre.dni .kalch (for Filimonov). (Spraying and dusting equipment)

DIBNER, Ye. E,V inzh.; FILIXONOV, S.-I., inzh.
Machanizatiow of the fumigation of soils in vineyarde. Zashch.
riot. ct Yzed. i bol, 5 no.10:15-17 0 160.
%IMIRA 26:1)
1. GosiLdarstvennoys spetaialluoye konatruktorskoye byuro
MaIdavskozo soveta, narodnogo khos"yetva, g. Kishinev.
(Phylloxera-Actemination) (Fumigation)

fN,R
Riki
gpg b MOW
/FWk(h) Pn
/E-w-(] Vmc
L u!
A 4,,4727
-noy
OCj
C P S 0
I Isill ~-Oshr-hnosteyv
e r Ot'
1964, 7-35
-r1O*
magnetron oscillator,
Im
theor)f, conttnuauls wave
-AGS: Oscil 113t0(
OF I C
fl, COL G~.
Continuous-
Iptlon or' ii I ch - Pawc r
ttie theory and descr
paper p 'esents
4 t
05 !a t.0 or. E - r CM
8 Je!
e4
7
4- F
T 77T 03
P,

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AT4c472,
'I'll - 7 v r, C.
i inn wh 1 ch takas place In a maqnetron. DurinQ over)tion of nIqo-
-io-,It,s ex r V~
LL
00 q[ R C1,109, P r"
D7 li PER: 00~

USSR/Human and Animal Physiology Digestion.
Abs Jour : Bel' Zhur - Biol., No 1: 1958, 4o64
Author : C.L. Filimnov
Inst
Title : An Apparatus for the Irrigation of the Stomach.
Orig Pub : Voyen.-med. zh-, 1957., No 5) 80-81
Abstract : A description is givnn of a simple apparatus for the
irrigation and ldvage of the stomach under field and
ai~bulatory conditions. The fluid gets into the sto-
mach throuCh one of the canals of the probe with the
help of a manual vacuum pump, and is evenly expelled
through another canal under the effect of the sane
PUMP.
Card 1/1
V-7
V

FILIXONO V, S.L 6~!:.Wvpilm)
Olive-Up made out of AIR-7 plastic for gastric bougles. Klin.med.
35 no.4:124 Ap 157. (KLRA 10:7)
(BOUGIM)
~,-t

FILIMONOV, S.S.
Iaborator7 investigations conducted on control of road sections
locat-9d in channels, Sbor, nauch. trud. po lesospl. no.2:95-110
'57. (MIT-d 11:7)
(Lumber--Tranaportation) (Hydraulic models)

GAVRILOV, Ye.N., inzh.; GONIK, A.A., kand. tekhn. nauk; DONSKOY,
I.P., kand. tekhn. naukj ZHUKOV, G.A., inzh.Cdeceased];
LAZ).,REV, M,P., inzh.; NEFEDOV, S.I., inzh.; PETROV,
Ya.P.J. kand. tekhn. nauk; SAVELIYEV, V.V., kand. tekhn.
inzh.; SHULITS, G.F., kand. tekhn.
naul:; ILILItj2NQV~ 5
,,j
naul:; ZOTOV, N.V., inzh., retsenzent; ORLOV, N.N., inzh.,
otv. red.; KOZLOV, A.D., red.izd-va; AXOPOVAt V.M.,
teklm. red.
[Water transportation of lumber] Vodnyi transport less;
spravochnik. Moskva, Goslesbumizdat, 1963. 560 p.
(MIRA 16:11)
(Lumber-Transportation)

V, T T I I-/ UI,j , 5 .
X LLI WITOIT
Plining Engineering
Dissertation: "Investigation of Heat Exchanee by Convection in flit,-h-Pressure Boiler
Furnaces." Cand Tech Sci, Po,,,,er Engineering Inst imeni G. M. Krzhizhanovskiy, Aced Sci
USSR, 5 Apr 54. (Vediernvays Moskva Moscov, 24 Mar 54)
SO: sum 213, 20 Sep 11?54

FILIMONa,941. kandidal tekhnicheakikh nmik; JUMSTALEY,B.A., kanclidat
~,--Ti),Kiicheskikh nauk: NOLCHUOGOVA,I.P., kandidat tekhnichaskikh
nauk
Experimental investigation of heat exchange in furnaces. Teplo-
energetika 2 no.7:30-33 JI'55- (MLRA 8:10)
1. Eney-getichoskiy institut Akademli nauk SSSR

KO.NAKCV, P.K., doktCr toki-nicherkL& rum~~; 17 IMONOV S.S., kandidat
n -f- tel-chnicheskikh nauk.
d I d r--'C
Calculation of heat exonange in boiier furnAces [with summAry in
(MLR.A JO: 9)
ng 11 E TeDloanorgetikn 4 no,;:4~'-53 Af, '57.
.,uticheskiy InstitILT Akademii nauk SbSR.
Rncirv
(Boilers) k'Heat--TransmiaBlon)

T -I, I
T 71 -,J rT
AUTHOR: KO.?fA]COV,P.K.,.PILIMONOV,S.S., KHRUSTALEV,B.L. P1 - 3562
,TITLEt On the Caloulaflo-n-o-f Radiative Heat Exchange in a Cooled Combustion
Chamber. (K rashetu luchistogo teploobmena v okhlazhdayemykh kame-
rakh goreniyat Russian)
PERIODICAL: Zhurnal Tekhn. Fiz., 1957, Vol 27, Nr 5, pp 1066 - 1075 (U.S.S.R.)
ABSTRACTt I scheme for the heat exchange process in combustion chambers iG
suggl)ated, which makes it possible to determine the required radi-
ation temperature TS and to calculate the radiation heat exchange.
It im assumed that near the heat absorbing surfaces there is a
layer of the medium which is in-equilibrium with radiation, the
mole,,.ular temperature of the medium and the radiation temperature
bein,5 equal to each other. It is assumed that on the way from the
balanoed layer to the wall radiation is not in interaction with
the medium, i.e. there is a transfer of radiation energy by effusinn.
It i;s therefore assumed that the temperature of this layer is
equal to the TS on the heat-absorbing surface. The temperature of
thebalanoed layer adjusts itself in accordance-with an interaction
between the medium and the radiation in the core of the flow.
The moleoular-kinetic temperature of the balanced layer is deter-
mined by means of a field analysis of the molecular temperatures
of the ignition chamber. Thum$ the balanced layer dicides the
Card 1/2 ignition chamber into two zones: one that is close against the

PA - 3562
On the Calculation of Radiative Heat Exchange in a Cooled
Combustion Chamber.
ASSOCIATION:
PRESENTED BTt
SUBMITTED:
AVAILABLE:
Card 2/2
wall and comprises the domain from the heat absorbing surface
to the balanced layer T he second zone, the medium core, comprises
the rest of the space: The existence of a radiation equilibrium
near the heat absorbing surfaces is proved theoretically and ex-
perinentally. The thickness of the balanced layer is measured
in millimeters. On the basis of what has been said it is possible
to dotermine the radiation temperature on the heat-absorbing sur-
face and to calculate the radiative heat exchange in the combustion
chamber. (With 10 illustrations and I Slavic references)
Inst."tute for Energetics "G.M.KRZHIZHANOVSKIY", Moscow
17.7.-1956
Library of Congress

4 ;-.4
MUSTALIVt B,,A,j FILDIDPOVj 3,69
Temporature field in combustion chambers. Teploonergetika (Ifnerg. Instj
no.1162-70 159* (MU 1312)
(Thermodynamics) (Furnaces)

2416o
Akad=173, rAUk Rnergeticheakly Inatitut IM"I
G. M. Krzhizhanovskly
TeploarAntilm, vyp. 1 1(Host Power EzgInvering. Nr 1) FIC8COw,
.d-V AN FS~R, 1939. 143 p. Errata slip inserted. go. or copies
printed not given.
94. of Publishing Houses V. A. Xotovj T~h_ Ed.: Tu. V. Rylloftj
2ditorlml Board. V. A. Baum, Doctor of Technical Sciences
Prof*esor Indsp. Ed.); 0. Ye. Kholodorskly. Doctor of TacAnical
Solencoxg X. 1. Yushchenkova, Candidate zf Technical Sciences
Z. L. Klrocllskly. Candidate or Technical Sciences (Secret&;"),
and S. 0. cyarkov, Cardidate of Technical Sciences.
PU9?MZ: This work is Intended for scientists and engineers working
In the field or stasm boilers.
COVER03: This is a collection of 9 articles on the circulation of
water and water.vapor mixture In boilers, bubbling processeso
a-
_j"tina of pressure. temperature fields In combustion chamber
radiation heat transfer uet- gr~q t=titt. --A the solution a
There is also-an
article describing proce.3363.0ccuring In the steam boiler of a
solar host energy stati . eferancen appear at the and of
each artl4l*.-.
;::j_-i:-d at thermohydrueloctric laboratories In cooperation
Elso~rlc Power r1s,
th Heat and 71r. No. 9.
0. 0. Vi kur V. ~, r-j9k21Wv. and
want nvestliji-joE Of Vappr and Got
Contents In & subblrz Process 40
It was round that the distribution of volume vapor content
Y and air content along the elevation or the bubbling volume
at Insignifloant'reduced veloaties or vapor or al.r. and at
low boiler water salt content, remains qualitatively the -
seas Lxz* virioug pressures and charaoteriatIca of the perforated
plate. An increase in the weight leval at atmospharlo
pressure results In a decrease of vapor content. An Increase In
the reduced velocity of steam when the water in of low salt
contant Increases the volume vapor content.
1. Pulsations of Pressure in tia Flow of Gas-Liquid
ixtarval Ix F"s 46
Mam artibl* describes *zparLmonte in pressure pulsation In
your 14* a long pipes or diffemnt dtamaters-23.8, 47-4. 74-7
and ".8 am. The flow velocity changed from 0.2 to sm/840.
The gas content changed from 0.05 to 0.95. Graphical repr*4*nt-
ation of' "parlowntal results are given.
NivaWl-akly. Z. L., and R. I. Sbayerova_ Investigation or a
Flow of Vapor Water Rixture In Pipes by r Radiation 53
I* tble article the authors describe problems In dater-
nbiln.g the average values of steas volune content* 9 av. In
p1p*s.and In condults of rea-tanitular cross *actlon. 'he
are &:..a .#'I'- for cenduitp r
arbitrary goomstrical shapes. Diagrams and graphs are given.
Khrustalev, B. Al and S. S. Pilizonov. Temperature Fields in
Combustion Chenbtwe 62
Three kinds or furnace heating Oftabers were Investigated.
B.pa.Isent&1 data,show that under cozaltion of approximate
**If-modell" temperature fields these -1-bern porform
according to load. It to stated tMt th: approxicato
Independence of dimensionless temperatur fields from the
rbdWoecurs in various combustion chambers which differ from
such Other according to geometric characteristics and the
type of,'Opsibu#tion processes.
Shohagoler, D. M. $than B011411 or 4 Solar jie&t Rnargy Station To
The author Drasaftts'dat.~
an tha yer-rcr=u%ce or st*am boilers
Operating On solar beat energy. Godaral diagrams of a
butler and tabies or Principa.L cheracteri.tic are given.
3urloove Tu. A. lavestitstlon of B"Ldtlao Heat Transfer in
Syste" or Gray Bodies 79
The author develops a theory of radiation ~tnd rallstion heat
t7m-M-Iftr, The sCuAtIOn4 &PpearIng In trAs article permit ,
thOOrstioal-probability interpreati_ ThQ t. di-
rid" Into two partal 1) Solution Of & mixed problem cc radj.
ALIon host 4xMVZ8 In 8 AY9bQa Of gray bodies in a diatherato
eadlum. and 2 Solution of &~ mixed prcb,~ez or radiation H&.t

jr
1p
2 F,~. lot
ar
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PF i's 1;
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is I

KOITAKOT. Petr KuzImich, prof., doktor tekhn.neuk; FILIMONOT,,Sergey
.Sergeyevich, kand.tekhn.nauk; KHRUSTAIZY, Boris Aleksandrovich,
k6nd.-6e-k-hn.nauk; ARNOLID, L.T., prof., retsenzent; LAKHMIIN,
T.T., prof.. doktor tekhn.nauk, nauchnyy red.; SWUNIKOYA,
Z.T., red.12d-va; BOMOVA, V.A., takhn.red.
(Heat exchange in the combustion chambers of steam boilers]
Teploobman v kamerakh agoraniis parovykh kotlov. Moskva, Izd-vo
"Rechnoi transport," 1960. 269 p. (MIRA 13:5)
(Boilers) (Purnaces)

32381
B/124/61/000/012/025/038
D237/D304
AUTHORS: Filimonov, S. S., and Khrustalev, B. A.
r------------ ;.-
TITLE: On calculating heat transfer and hydraulic
drag in the laminar flow of fluid in tubes
PERIODICAL: Referativnyy zhurnal Mekhanika, no. 12, 19619
95, abstract 12B655 ~V sb. Konvektivn. i
luchistyy teploobmen. M., AN SSSR, 1960, 221-
232)
TEXT: The method of processing experimental data is given, V~
allowing the calculations of local and mean characteristics of
heat transfer and hydraulic resistance in laminar flow of fluids
in tubes heated in a constant flow of heat under the condition
of simultaneous development of thermal and hydrodynamic boun-
dary layers. It is shown that the dependence of the Nusselt
No. on Gretz criterion,
Card 1/4

32381
S/12 61/000/012/025/038
On calculating heat... D237YD304
Nfx f (Gz')
qd x/d (1)
N t.VM - tfX ) hfx Gz? PI f
does not fully reflect the influence of all parameters on the
mode of developmentt as the spread over the layer'of experimen-
tal points depends on the magnitude of thermal flow q on the
temperature of the fluid on entering the experimental region,
The author succeeded in representing the experimental data by
fX PWX 1/3 4.36 + 0.36 X-1/2 10-18X (2)
( PfX
Card 2/4
4'.

S132351
124/61/000/012/025/038
On calculatine; heat... D237/D304
which enables the calculation of the wall temperature at any
point of the tube under the condition of constant thermal flow
with simultaneous formation of thermal and hydrodynamic boun-
dary layers. Graphs of XfX (P WX / P fx) 1/3 v. X are given for
the experimental data of various authors. A formula is proposed
for the determination of the region of thermal stability, and
a graph is given of the mean Nusselt No. N v. mean value of
the criterium, X. Experimental data on hydraulic resistance
for the front part of the tube ~(x/d) R f1 0,065 are satis-
factorily described by
~X RI ( x/JdO-56 -14.6 -x/d
'I = 4 + 3.2 10 (3)
175'
R'
(PwX/Pfx) f
Card 3/4

32381
,/61/000/012/025/038
S/124
On calculatinE; heat ... D237/D304
Graphs are given of the change of local and mean coefficients
of hydraulic resistance v. the criterium x/dRf 0, and a formula
is given for determining the initial hydrodynamic region. Z-Ab- /
stracter's note: Complete turanslation-2
Card 4/4

S/057j6O/O3O/O6/15/023
6~~'o 0 B012/Bo64 81594
AUTHORS: Tilimon Khrustalev, B. A., Adrianov, V. N.
WWeA7F11A4Wffl19,7 ~ 07 7H
TITLE: On the Theoretical Principles of the Method of the Two
-aadiometere lo
It
PERIODICAL; Zhurnal tekhnicheekoy fiziki, 1960p Vol, 30t No. 6,
pp. 690-698
TEXT: V. S. Kocho (Ref. 1) introduced a method for the separate measure-
ment of the rs.diaticn flow and the convective flolf (method of two radio-
meters)* This was used in the investigation of the heat exchange in the
Siemens-Martizi furnaces (Ref. 1) and in the combustion chambers (Refs. 2, 3).
In the present paper this method is analyzed. The beat absorption at the
relevant plaon of heating is measured simultaneously by means of two radio-
meters with diff erent degrees of blackening A, 9 A2' of the heat-absorbing
01_-~Grlts. The formulae (1) and (2) are written down for the calculation of
the heating flow. It is assumed that the density Eincident of the incident
radiation is 9qual for both radiometers. Furthermore, it is assumed that
Ca-r -1 1./,5

On the Theoretical Principles of the Method 8/057/60/030/06/15/023 8159h
of the Two RadLometers B012/BO64
the convective flows for both radiometers are equal and - q k. Formula (5)
is derived for Eincident and (6) for qk which are commonly used in calcula-
tionso The conotancy of E incident Is maintained if the measuring surface of
the radiometer is considerably smaller than the over-all surface of the
heat exchanger,, In order to prove the accuracy of the assumption of the
mutual independence of the convective and the radiation current the experi.-
mental investigation described herein was carried out. This was done by
means of 3 radiometerse This proof was based or. the idea that, if the
assumption was right, any pair of radiometers would yield the same results
as the other two pairs. The investigation showed that the hypothesis of tho
mutual independence of the radiation flow and the convective flow in the
medium boundary layer in the combustion chambersis in practice maintained
with sufficient accuracy. The experiments have shown that by the method of
two radiometers and by fulfilling the conditions
A2 < 0.2 and Fradiometer <
Al Pheating-
I satisfactory results were obtained.
Card 2/3

On the Theoretical Principles of the Method S/05 60/030/06/15/023 81594
of the Two Radiometers BO12YBo64
This should alsio be considered in the production of the radiometers, In
the present paper also a mathematical analysis of the accuracy of formulas
(5) and (6) wav carried out on the basis of the error theory. The two
methods applicable in this case(ar~ given. On the basis of this analysis
formulas (10), (11)9 (12), and 13 were derived. With theso formulas all
the extreme relative errors in the required quantities can be calculated
in dependence of,all the factors influencing such quantities. The analysis
showed that th-a errors 6Eincident and 6qkdiminish with decreasing ratio
A2
-onfirmed by the results obtained from the experimental in-
A This was
vestigation. There are 6 figures and 4 Soviet references.
SUBMITTED: November 18, 1957
Ca:~_' 3/3

FILIMMOVI S.-S-1 and MMTALEVp B. A.
"Evaluation of Local Heat Transfer and Hydraulic Resistance
at Turbulent Flow of Water in Tubes with Different Inlets."
Report submitted for the Conference on Heat and Mass Transfer,
Minsk, BSSR, -une 1961.
A"';
~N

ACCESSION NR: AP4004156 S/0294/63/001/00210318/0320
AUT11OR., Kryukov a, It., G. Tep I ov, S . V. ; Ayf'istov,
A. A.
TITLE: Test stand for studying heat transfer i.n.the flow of liquid
aluminum in a pipe
SOURCE: Teplofizika vy*sokikh temperatur, v. I's no. 2, 1963,
318-320
TOPIC TAGS: heat transfer, liquid aluminum he'at.,ex changer, liquid
metal, liquid aluminum, aluminum heat.transfer, heat exchanger,
liquid metal coolant, coolant, fluid flow
ABSTRACTiI A test, stand has been designecb for heat-transfer studies
with liquid aluminum. The use of liquid,aluminum as a heat-trans-
fer agent in heat exchangers operatiing qt temperaturesexceeding
1200C is being investigated since difficulties are encountered
with alkali metals at such temperaturea. Fig. .1 of the Enclosure
shows the test assembly. An induction-type"electromagnetic pump
with a traveling magnetic field (capacity 3 m3/hr) was speciall7
Card113 '*kl~

ACCESSION M AP4004156
.'developed for the assembly. Two types of heating.can be used: an
electric~nichrome heater which will-heat the pipe uniformly at a
of 5 x 106 kcal/m2thr, or an electron bombardment heater,
heat flux
which will give higher heat fluxes. Thermal expansi.pn of the graphite
parts is.conipensated by means of sylphon expansion Joints. All parts
of the assembly in contact with the nluminum are made from pyrolytic
g ra ph i t c.0- Preliminary testing for 200 hr with individual test iuns
..of up to 12--hr duration showed the design to be sat0factory and the'
assembly au.:'6table for heat transfer st.udies. Orig. art. hns: I
f igure
ASSOCIATION: Energeticheskiy institut in. G. M. Krzihizhanovsko~o
.(Power Enginee-ring Institute)
SUBMITTED: 15Apt6j DATE ACQ: --26Dec63 ENCL: 01
SUB CODE: PR NO REF SOV: 00.0 OTHER: 000,
Card

'/kpl~r
4 /P s -4/Pt -1101, P'Li-Al T~M
IN R AP50 01154 ZD (p) - 3 M/MV JG 5 .2 9 4 D 1_'; D .1 0 1 0 9 C~ 9
S. S. ; KrEukova, M. Teplov S - V
AU"HOR: Fj,k~j~ ~r~!g ~'-
Ift
TIME Inveistigating hcat transferrin pipe flow of liquid,, Uunirium_
temperaturt 4, 901-909-7
SOURCE: Tciplofizilka VyHokikh v.- 2 , no . 6. l4t'
T 0 P I Cl 7' A 11; 3heat transi~er agent, liquid metmlt heat transfer, aluminum
ABSTRACT Tie Krz*hizhanovskiy Power Institute in-..,e,;tjgsted
the I e it transfer 'In a spire flow of 11 qui a I imi nurr. a view
1:- n - ii ~1 al u-ni num as a h i -h- ternnne -it urt- Anc to )olant.
e i t 9 ve re ~Cr durte (j %., I t r, a Q - 19
aluminum in a specially rp cr- t c -I
1~ Be ct i on cons i sted of an e iect r- r a P'n i t e
1~! e. Flow rate and temperature of aluminum at ~.nt~ inir-. a P, (i outlet
o f the test sectiun and the vall temperatureG werc mca!3ur,zd u,ider
steady-state conditions vith turbulent flow and uniform hee,.t supply
to the tent section. The heat transfer coefficient was determined
from plots or the insido-surface temperature or the pipe veraus the
r-ean calorimetric temperature of aluminum &t EL f;iven cross section.
Card

L 18398-65
ACCESSION M. AP500-1154
The experimental dat ain terms of R u and Pe numbers are preaeated in
Fig. I of the, Enclosureaiong with t-he results of other favest1gatcrs
for heat travs-re-r- low- A:kk-. all -i mete-.'
tEinad are vtt 11 deacribed by, the equation Nu = 5 4- 3, 'd aerived-
b%; revere-1 aitthors on the basia of experimental d&ta for hcat tr&asfer
in turbUlent J.'lov of alkali metals and mercury. Orig. art. tiou., 7
formulas, 1 -.&ble, and 3 figures.

i., , , ; ~ , ~~ ir ..
J,-, - --,,
wocd idgrinf, lumbur P~-ul..
IV:);*,* J Lpkh. 1~ifcjr:n. 17 no.9:55-58
,~ 16~- ( l.: " ?"'. 18:1)

FILIMONOV) Sergoy Sergoyevich; FOTAPOV, Fedor Andreyovich
(Felling and floating birch timber) Zagotovka i spla.
drevesiror berezy. Moskva, Lesnala promyshlennost',
1965. 72 p. (MI RA 19: 1)

Mai: "r
ACC Nit, AP602650 CODE: UR/0118/66/000/005./0016/0018
AUTHOR: Verte, L. A. (Candidate of technical sciences); Filimonov, S. S.
;(Candidate of technical sciences)
:ORG: none
!TITLE: Induction. pump for liquid aluminum
!SOURCE: Mekhwiizatsiyaiavtomatizatsiyaproizvodstva, no. 5, 1966, 16-18
!TOPIC TAGS: liquid metal pump, electromagnetic pump
IABSTRACT: In 1961, a new induction pump was developed for the purpose of circu-.,
I
.lating liquid aluminum through an experimental heat-exchange circuit a:t the Power-
!
Engineering Institute irn.Krzhizhanovskiy. The pump's essential parts (see figure)
Are: 1-housing, 2-magnets, 3-three-phasewi 'ndings made from cooling-watdr-
carrying copper tubing, 4 - aluminum-carrying graphite channel, 5 - starting heaters,
i6 - graphite connection nipples. The pump has a capacity of 0. 195x 10 3 m3/sec and
!develops a Pre89VLr0 of I kg/cm', phase voltage, about 45 v. The pump has had over
130 operations; overall working time, 150 hra. Orig. art. has: 2 figures and 1 table.
1/z UDC: 621.65/68:656.546

CODE: 131 09 SUBM DATE: none
-2/2
026505

D
~~LTCjjj&,* Q/ETI IJP(c) JH/j1V U / U
ACC NR: AT6029312 SOURCE CODE: UR/0000/66/000/000/0068/0083
AUTHOR: Filimonov, S. S.; Kryukova, M. G.; Teplov, S. V.
ORG: Power Engineering Institute im. G. IM. Krzhizhanovskiy (Enegeticheskiy institut)i
TITLE: Alum:'Lnum as a high temperature coolant
SOURCE: Mosilow. Energeticheskiy institut. Teploobmen v elementakh energeticheskikh
ustanovok (Heat exchange in power installation units). Moscow, Izd-vo Nauka, 1966,
68-83 f
TOPIC TAGS: highnz=qmxature reactor, reaetei-e6b1ing, nuclear reactor, reactor
A, ..V'T-I-e
coolant, -1+i~ild-metaL cooling, aluminum cvo4idQ:.,-t1L7qu4,(6*~m, liquid a4"wA-a~jm
ABSTRACT: Since 1959, the Power Engineering Institu%(! im. G. M. Krzhizhanovskiy haq
been engaged in a study dealing with the use ofl~iqHLid aluminum as a coolant fori
high temperal:ure nuclear reactors. The experimental equipTrent and some of the
results of this study are described. From the study, it was concluded that the
difficulties encountered in the practical use of aluminum as a coolant can be suc- i
cessfully overcome, and that the heat transfer during the flow of liquid aluminum
through pipeii can be calculated With the equations uqed for calculaLirg the heat
transfer of other liquid metal coolants. Ori.g. art. has: 4 figures and 5 tables.[MI
SUB CODE: 13/ SUBIM DATE: 05Apr66/ ORIG REF: 016/ 0111 REF: 008/ ATD PRESS:5069,
Card 1/i ML~- I . - i

VECHTUM) inzh.; KUDIRYAWMEV, V.A., inzh.; MALKES, D.A., in--h.;
OSTROVOKIYj G.I.;POVERENNYY, L.D.;SUSIIKOV, P.M., inzh.;
IYUMMV, V.Z., inzh. Prinimali uchaBtiye: GALYA:~.'OVA, N.S.., inzh.;
FUTMVA, N.P.; IZRAYLOVICH, Ye.A., inzh.; MAIRCIU21KO, G.A., inzh.;
MMYGMA) Z.S.; SOKOLOVA, Ye.A.; SONOV) V.11., inzh.; TARASOVA,
S.N.; TASHAYEV, A.L., inzh.; EI SX-j-D11ALICH, K.F.,inzh.,
nauch. red.; NOVITCHENKO, K.M., inzh., nauclinyy red.; SI1.1AKOV,
S.N., -Lnzh., nauchnyy red.; FAKTOROVICH, Yu.A.., kand. tekhn. nauk,
nauchniry red.; STUPB4, Ye.N., otv. red.; LUTOV, N.S.,, red.;
IVANOV) V.S., red.; BAGUZOV 1T.P glav. red.; VOLCIIEGORSKIY, M.S.)
Y -P 15
zam. glav. red.; DOBRY111IIs, S.N., red.; NAZAROV, I.A., red.;
KOLESNIKOV, S.L., red.; IMLINIKOV, III.P., red.; SUSITIKOV, A.A.,red.;
STAROVIMOV, I.G., red.; IYTKITIA, L.S., red. izd-va; GUZEYEV, P.A.,
red. izd-va; OSRTKO~ L.M., teklin. D,,d.
(Handbookfor the designer of industrialp residential, and public
buildings and structures; organization of construction and execu-
tion of building and assembly operations. Industrial construc-
tion] Spravochnik proektirovshchika promyshlenrWl:h, zhilykh i
obshchastvenrq1ch zdanii i sooruzhenii; organizatsiia stroitell-
stva i.proizvodstvo stroitellno-nontazIuWkIi rabot. Promyshlon-
noe stroitollstvo. Pod red. P.14.2ushkova. 1"lookwa, Gos.izd-vo
lit-ry po stroit., arkhit. i stroit. imteriaLaw,, 1961. 372 p.
(MIRA 15:2)
(Industrial Imildirv,s)
.1

BUKSHTM , D.I.; AFANASIYEVA, A.A.; MIKHATLOV, V.O.; SUSHKOV, P.M.;
.~g7LIMONOVIC.A.7,; ROZRDESTVENSKIT, I.I.; GBRASIMOVA, G,.S.,
red. vis; RUDAKOVA, N.I., tekhn.red.
Dethods and norms for determining rated costs of and labor
riquired in making precast reinforced concrete construction
elements] Ketodika i normativy dlia opredislonlia raschatuoi
stoimosti i trudoemkosti sbornykh zhelezobatonnykh konstraktaii
nit stadil ikh proaktirovaniia. Moskys, Goa.izd-vo lit-ry po
ittrolt., arkhit. i stroit,materialem. 1960. 62 p.
(KIRA 13:6)
L, Moscow. Gosudaretvannyy inatitut tipovogo proyaktirovaniya i
toklmicheskikh iaeledovaniy. 2. Inatitut- okonomiki stroitel'stva
Qor Bukuhtsyn, Afanaelyeva). 3. Institut betona i zhelazobetona
Uor Mikhaylov). 4. Gosudarstvennyy institut tipovogo proakti-
rovaniya i takhnichookikh issladoveniy (Giprotia) (for Sushkov,
ftlimonoT, Rozhdastvanskiy).
(Construction industry--Costa)

FILIMDNOV, S,To.
I
6
Now order for estimating in railroad construction. Transp.stroi. 6
no-3:23-24 Kr '56. (=A 947)
l.GlavVy spetsialist otdola Gipropromt:ransatroya.
(Rairoads--Cost of construction)

FILIMONOV 5 Y Inshener, otvatetvennyy red.; PSVZM , A.S., red.lzdatelletya;
8.S., takhn.red.
[001140tion of suppl"ents, eluci4$ions, and amendments pertaining
to the w4form distT~4t prices] qoqrnik dopolnenii, rasliasnenii
i poprAvok k edin" r#iowVm edifichnym rasteenkam. Moskva, Gos.
iz&-vo lit,-ry po stroit.i arkh~ ,.
1957. 94 P. (MIRA 10:12)
1. Russia (1923- U.S.S.R.) (kqqudarstvennyk komitet po delam
stroitelletva.
(Building materials--Cost)

FILIKOHOIN &B. inzh., rod.; PWZNXR, A.B., red.izd-va; SOLUTSZVA,
In. F-T%0;I;.red*
[Collection of additions. explanations, and corrections to
standard district rates] Sbornik dopolnenii, raz"iasnanii
:L popravok k odinym raionnym adini.chnym rasteenkam. Moskva,
3os.izd-vo lit-ry po stroit., arkhit. I stroit.materialem.
:9o.2. 1958. 37 P. (MIRA 12:9)
1. Russia (1923- U.S.S.R.) Goaudarstvannyy komitat po delam
stroitalletva.
(Building-Ratim3tes)

CHEIUTYSEIIIV, Petr Georgiyevich; FILIMONOV, Semen Ye
RUSMOV,
ll!.kolay Vasillyovich [c " - 0
lec-eil36Vj;"VVM',-Alekaandr Rodionovich;
KIUSRTALI, L.I., red.; BOBROVA, Ye.N., tekhn.red.
Ellatimates, bookkeeping, and technical records in construction
and track: management] Smety, uchet i tekhnicheaksia otchetnost'
v stroitelletve i putevom khoziaistve. Pod obshchei red. P.G.
Clieraysheiva. Koskva, Gos.tranap.zliel-dor.itd-vo, 1959. 235
(MIRA 12:939
(Railroads-Accounts, bookkeeping, etc.)

otv,red.; RUMKOVA. N.I.. tekhn.red.
(Additione.0 explanations, and/corrections to standard district
rates for building work] Sbornik dopolnenii, ratmiasnanii i
popravok k edinym raionnym adinichnym rasteenknm na stroitellnye
raboty. Moskva, Goo.lod-vo lit-ry po stroit., arkhit. i stroit.
malmrialam. No.3. 1960. 463 p. (MIRA 13:7)
1, Russia (192)- U,5#5,Ro) Goaudarvtvenayy komitat po delam
stroitalliltva.
(Building--Zotimates)

MMUGIll, V.I.; YEFfM-'OVj S.A., kand. tekhri. nauk; R MD.', S.11.;
BUKSMYR, D.I.; DUNAYEV, Ye.S.; KILI, AM.; KHAKOVICH,
L. A. ; FILD101'4QV,.$.Ye.; PETROV, I.A., prrof., doktor
l,ekhn. nauk, nauchn. red.; GIHOVSKIY, V.F., prof., doktor
ckon. nauk, nauchn. red.; GERASIMOVA, G.S., red. izd-va;
WLIBERG, T.M., tekhn. red.
[Manual for estimated costs in cont3truction] Spravochnik
po smatnomu. dolu v stroitellstve. IToskva, Gosstroii--dat,
11t.2. 3-963. 462 p. (MIRh 16:12)
I. Akademiya stroitellstva i arkhitektury SSM. llauchno-
Lssledovatellskiy institut ekonomiki stroitellstva.
(Construction industry-Costs)

DESEYATNIK, E.N., irwh., red.; YELISEYEVA, Yo.Ye., in-li., rcd.;
v.u~'Jt.3iiov, A.G., inzh., red.; GUIZV, V.I., -Lnzh., red.;
t"ALAKROV, A.Ye., inzh., red.; PETROV, G.F., inzh., red.;
:FILL.011OV, S.Ye.p inzli., red.; ROKKO, li.A., lnzll rod.;
t.u. inzh., red.; E.A., -.nzh., red
LE10--KOll, A.D., inzh.0 red.'
(GollocLiolls 1108. 10, ')(), 31, ank"i /,2 of qUin6ard dtsu-ict
-iniforril r-stiraites for conotruction worl I Jwrnil'l 1:0.10,
210, 31 1 42 edipykYj ralorMkh ociinichnykIll rajt~:c-nok na
stroitellni.re raboty. Poskva, 3troiiaint, 1965.
(vr.u"t 18:10)
1. hu,-~sia (1923- U.S.3 Gosudarntvevn~pkomitet po die-
lam stroitellstva. 2. Gosstroy SSER (for Desyatrik, Guscv,
Fili-monov). 3. Ilauchnf)-issledovatellskiy institiat akonomiki
struitollstva Goostroya SST-, (forYolineyeva, I-11irashov,
I:iokko, Andreyov, Fialak-hov, Turianskiy). 4-Cosudarst7cmyy Eoyuz-
my institut po proyaktirovaniyu --pet.3ial-''l'.ykli ,oo,-uzheiily, -daniy,
sanitarno-teklinicheskikh i energeticheskikh ust---o- '- rllvq nvedpri-
yatly khimichcokay pron~:shlmmsti(fcr Fetrov). WSentralhWy
nauchno-iosledovatellskiy i
.1 in.,titut
promyshlennykii zdariiy i soo-Aizheniy (for Zerenkov).

SOV/84-58-10-5/54
AUTHOR: Filimono,
TITLE: Labor Duty (Trudovaya vakhta)
PERIODICAL: Grazhdanskaya aviatsiya, 1958, Nr 10,*r 5 (USSR)
ABSTRACT; 7he author tells of the pledge to fulfill. the annual plan
by 18 December [1959). i.e., ahead of schedule, made by the crews
in his tLiit in honor of the XXI KPSS Congress. The Red Banner
challenge prize hadin the past 8 monthsbeen awsLrded twice to the
personnel of the unit for superior perfoniance by the Main
Administration of the Air Fleet (GUGVF) and the Central Committee
of the Union of Aviation Workers (Soyuz airiarabotnikov).
C arl 1.11
R,

FILIMONOVP V.
Wo:7k program of meteorological posts. Meteor. i g1drol. no.10;
47 0 '61. (MIRA 14;9)
(Tuva Autonomous Provinca--M(itearology--Observations)

7ILIHOIIC,V V 1% . Kharlkov),
Using, indicators. Fig. v shkole 17 no.3:67-69- MY-Jo 157.
(Measuring instrunents) (MLRA 10:6)

on
V.I., insh.; LMUCHIV, A.S., inzh.; LUNWICH, H.V., inzh.;
MMVITIV, I.N., insh.; FILIMOROV, V.A. , Inzho
Public utilities and coymmunications In a satellite city
near Moscow. Gor.ichos.Kook. 34 no.4:10-13 AP 160*
(KNA 13: (1)
(Kryukovo--Citjr planning)
(Eryukovo-severage)
"N

,.Kjyp V4,kof inzho; FILDIONOV9 V*A*j inzh.
ZELENEVS -
*Ways of improving the planning of angineerimg com=aications in
Moscow. Gorekhols*MOSk. 36 no.6.19-22 J41 162. (IUM 15-8)
(moscow-112nicipal engineering)

gram
110.
'-Shy pmd the awl rumvn of t5, 'Id"M
RA kl'o
M T-T,
T~4 e-Nn~# iof the nWkj f, Ca~_
USIL
betcen t=- ~~
~!Cr-s vj" I .
diff=nt exchan., charactV's fOr ~-,p and t~fj fi~~,,er-
acti-I. C-1=b [a.= am d:rA
is then taken ai p - 71 fty
17" ror r -- Z n-,:1 P,
& and t4cncq~ii;lnldjl-,
with fnlcpcn&,nt lized.
accUr.
ring here. V111th the rmulting chargc density c!zml.
ponk&3 With a, #iVe., anguf" ",cf,
'd and the number (3( P3ri:cki lyl iA 1:3 kutt fed
AS 2 fUnctian ar Cum btr of nucreong.
P4
MMM
jR

USSR/Nuclear Physics - Nuclear shells FD-236o
FILMONOV 'V. A,
Card 1/1 'Rib. 146 - 25/34
Author : Filimonav, V. A.
%wUwXUV" I ~ i4!' I
WX 0 ~%
Title : Deviations oimmt~ s scheme in the filling of the shells of a
Ir e r
nucleus and in the interaction of thelevels
Periodical : Zhur. eksp. i teor. fiz. 28, 753, Jun 1955
Abstract : N.. I. Korsunskiy (Uspekhi fiz. nauk, 52, 1954) pointed out that in
the Mayer scheme of filling of nuclear shelln there are nuclei
that do not build up their levels according to this scheme. The
lirespnt author explains this departuare on the esample of 23Vall
e,nd '?5Mn25-
Institution : ?Iariinskiy Posad Forestry Engineering Technicum'*
Submitted : June 26, 1954
Mariinskoposwiskiy lesotekhnicheskiy tekhnikum

LYAMIN, A,;A,, inzh.-, ZAKHARMO, S.Ye., inzh.; STIALINOV, A.F., kand.
tehhn.naulr; YUSHKIN, A.R., inzh.; FILIMONOV, V.A.i inzh.
OSTA11TSEV, P.P.
Tho technical and economic expedienc7 of the simultaneous
int3tallation of underground equipment b7 engineering teams.
Gw.khoz.14ooke 31 noollt30-35 N 157, (VIRA 10:12)
101osenergopro7ekt (for Iqamin). 2.Mosteplonotletro7 (for Zakhar-
chunko). 3.Mospodzemproyekt (for Shallnov, Yushkin, Filimonov,
Ostalltaer)
(Municipal engineering)

21(l), 21M. 24M
AUTHORi Filimonov, V.A. SOV/155-58-2-38/47
TITLE: _2~_-Ifu,-Ton -Forces and the Binding Energy of the A-Particle in
Light Hype= 3.ej ( A -nuklonny 8 sily i energiya svyazi A -
chastitay v legkikh giperyadri ~
PERIODICAL: 3auchnKye doklady vysshey shkoly. Fiziko-matematichaskiye nauki,
1958, r 2, pp 174-180 (USSR)
ABSTRACT: The author starts from the Lagrangian of the reciprocation of
barions with 1~and K-meson fields according to Espagnat and
Prentki ZRef 67 and calculates the forces between a A -particle
and a nuclon combined with the exchange of one K-, two 7-mesons,
two ?c - and K- and It-mesons. The obtained forces are used in
order to calculate the energies of the hyperkernels AH3 , AH4
AHe4 and AHe5 . These theoretical results show a good agree-
ment with the experimental results. The author thanks Professor
D.Ivanenko for bla assistance.
There are 9 references, 2 of which are Soviet, 4 American,
2 Italian, and 1 English.
Card 112

A-Huclon For,,,es and the Binding Energy of the S0055-58-2-38/47
A-Particle in Light HyperMWlei
ASSOCIATIONiMaskovskiy gosudaretvennyy universitet imeni M.V.Lomonosova
(Woscow State University imeni M.V.Lomoposov)
SUBMITTED: January 5, 1958
Card 2/2

AUTHOR: Filimonov, V. A. SOV/48-22-8-20/20
TITLE: -Nucleon Forces an article Binding Energies in
Hypernuclei (A-nuklonnyye sily i energiya svyazi--iV-chastitsy
v giperyadrakh)
PERIODICAL: Izvestiya Akademii nauk SSSR, Seriya fizicheskayal 1956,
Vol. 22, Nr 8, pp. 1009 - 1012 (USSR)
ABSTRACT: The J'.-nuoleon forces were computed by the author in a similar
manner as the nucleon-nucleon forcea- in the paper given by re-
ference 2. The matrices Aand transform the.~~-particle into
a nucleon and vice versa. The author formally considers the
A-particle and the nucleon as to represent two different sl.ates
of the baryon. They are described by a one-column matrix:
11
A
0l
; -
N -1
--j
0, 1
In order to compute the A-particle binding energy in the
hypernucleus the interaction potential energy between the
nucleon in the core of the nucleus and the ~'~--particle in the
) state is wanted. The part
) and in the singlet (E
triplet (E
s
tr
Card 1/4 of the forces independent of the spin contributes to the potential

30V/48-22-8-20/'20
-A-Nucleon Porces and the -~'-Particle Binding Energies in Hypernuclei
energy of the triplet and of the singlet state, which have
equal values, yet opposite signs., The potential energy of
different states differs considerably. It is negative for the
singlet and positive for the triplet state. In both cases it
has approximately the same absolut value. Hence it can be
concluded that the state preferred by the 2,w-nucleon pai-r is
the einglet state. Therefore in light hypernuclei states with
the greatest variety of singlet pairs wil' ' have -?he smal.Lest
energy. That is to say the ground state of light hypernuclei
will be that with the smallest spin. In this case the -A.-
particle potential energy in the hypernucleus is given by:
3 E I E + .1 E
H p 2 a 2 tr;
4 He4 I!, I E + I E
? 2 8 2 tr
\~ He5 Ep Ea + 3Etr'
Card 2/4

SOV148-22-8-20120
-A-Nucleon Yorces and the -it-Particle Binding Energies in Hypernuclei
The kinetio ernergy is~klwn by the equation:
1 2 mn 2
Ek - 8 Al - 2 mno
M 1~, 4-
The computation of the function of the energy verausq by
numerical intergration of the formulae (17) - (19) proves to
be very easy. The smallest value of the -1-particle binding
energy B.& - - E min can also easily be determined. Results of
such a computation are given in a table. They show good agree-
ment with experimental data. Por g2 , however, cL smaller value
must be taken as proceeds from the data on the nuoleon-nualeon
forces. There are I table and 3 references, 0 of which is
Soviet.
ASSOCIATION: Kafedra statisticheskoy fiziki i mekhaniki fizicheskogo fakult-
teta Moskovskago gos. universiteta im. M. V. Lomonoanva
(Chair of Statistical Physics and Mechanics at th,_~ Physics Depart-
Card 3/4 runt of the Moscow State University imeni M. V. Lomonosov)

SOV/46-22-8-20/20
-/I-Nucleon Forces and the -A-Particle Binding Energies in Hypernuclei
Card 4/4
uscomm-Dc-6w,83

AUTHOR: Fillmonov, V. A. SOV/56-34-5-61/61
TITLE: "_~e _'~_-Nucl`son P'otential According to the Meson Theory and
the Energy of the J-Particle in Light Hyper-Nuclei
(,'-muklonnyy potentsiall iz mezonnoy teorii i energiya
,'-chastitsy v legkikh giper-yadrakh)
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheakoy fiziki, 1958
Vol. 34, Nr 5, PP. 1355 1356 (USSR)
ABSTRACT: The interaction of the- .-particle with the nucleons in the
nucleus is connected with the low energy range. It may there-
fore be expected that the-1--nucleon potential derived from
the theory with cutting off (with respect to the momenta) of
the virtual mesons will give reasonable results. The author
calculated the --nucleon potenzial, using an interaction
Hamiltorian, which is given explicitly in this paper. This
Hamiltonian can be derived from the interaction of baryons
with pion fields and K-meson fields using.a Dyson trans-
formation. Moreover it in assumed that all constant bindings
are identical. Using the above-mentioned Hamiltonian, the
author calculated the fornes between/ and nucleons coupled
Card 1/3 by interaction with one K-, two n and also with two K-mesons.

SOV/56-34-5-61/6i
The J/-Nucleon Potentiv-1 According to the Mesoa Theory and the Energy
of the .-Particle in Light Hyper-Nuclei
The calculated forces were nsed to find the binding energy
of the light hyper-nuclei jH3, H4 I H5. The potential
energy of the -,.'-particle (which is bound with 2 n-- and
2 K- meson forces) in n. hyper-nucleus hardly depends on the
spin of the hyper-nucleus. The potential energy due to the
I K- meson forces amounts to 1/10 of the whole potential energy;
it is positive and approximately the same for all light
hyper-nuclei. The low value of the 1 K- meson forces is due
to the non-monotonous potential of these forces. The energy
due to the 1 K- meson forces depends very much on the spin
of the hyper-nucleus. The lowest potential energy cor-
responds to the smallest spin values of the hyper-nuclei.,
Some numerical values are then given. The theory discussed
in this paper gives binding energies which lie too close~,~.
together. AlthouCh there is no quantitative agreement the
discussed theory correctly states that the forces betwe*en
and nucleons are not pure 'Xigner (Vigner) forces. The
Card 2/3 author thanks Professor D. D. Ivanenko for his help in

SOV/56-34-5-61/61
The //-Nucleon Potential According to the Meson Theory and the Energy
of the -',-Particle in Light Hyper-Nuclei
carryine out of the discussed investigations. There are
5 references,
ASSOCIATION: Moskovskiy gosudaretvannyy univorsitet (Moscow State
University)
3UB,AIV23D:: January 15, 1950
1. Nuclei-Energy 2. Paittioles--Enerv 3. VABons--Theor7
4. Nuclear spine 5. Mathematics--Applications
Card 3/3

-)f L il-" t
C..... t 0
discussed ii
t 0:7~:.L C I I " 1::r t 1C, L, t
s 3 u f
"'y t
1: 1 V T" I
b in.' i rt 1
c~r me,-nz of 7c,3,-j:. i,-.)c.,
Cor. of
-A b.,., ry 0 7 Viithout 0.- ~~ny -0 t:.,
C a I/ y of

of Li,-..t
1.,;cd vi~.u;-. dv,.Iiii~..
t t
df,~vol,)~jcd 'by Pilim-mov in or (RcIf
11 01
on a~;:,imltion t'., t t'-.,, r:c i o
1 t sfor bar,
+
of
tile for t~.,: Iko -c,
L
;I I, I tn d ovin i,; - Is- urao ~rrc
zero. F1,,r-t'.c_--:.-,urc, for t`.,~ intlerac"_icn
..:-.cl -triplI.A0 fov t (I c a . 7it
t',. ei d o ' t'l c r ec 14.- z o f r e
of t"eA
Hr_,4,
1/2, 0, 0, 1/2' t'.eorly L! 2.
order)' "'.;t."
Card 214 E 3 2 2~
kin' (M /M, y J:~I c '),"0 0'~t
71 A 5

E
I C: ,
,u Bindizi~; Ener~;j of' Lij,711,it H--i:~-rnuclci ccoL,jiI,,r ,o
t.- ' .1 A .1
e -,
coor, T, eor
3 J1 1 K 2K
E = E + 2E + E 5 EK% + 2E
1-in c c 3 c
4 4 2n ZU. 2K
H 11,-~ E= E + 7E 2E" + 7,E
kin c c
e:) 2 1 K. K% 2K
E= E, + 4 F, 2 E E + 4E
:ill c c C c
C~Ilcld,~tion rcovzltk:3 ott.-.inud b.,r u,-.in,- tlie -1 2_
of rc~f",.,Q;Xe 4 -.re -`-o-un in a :,,-,blc,.
rzwulto :,.rc, fcun~! to lic in
,,-:!rimcnt-,1 ones. In coi-.---Iu.-ion thc-
D.D.Iv,--ncriko for his L, t th 4 o
I ~ ': o JI
Tner.- arr. 1 table :-~nd 1~: 2 c'L wilich are
s:w-i"A .
ASSOCIATION: Moo::ov2'~:iy gooudarctvcn:~yy S--~te
univurcity)
Card 3/4

1 rr
04 t.
00
-,sos It
IZZ R c-
91
t - - :k :1 ?. o
3 -or I ~ 2. 4J?p4~0 as 'a Via
tI a r. 1.
'0 a
-08
2 1.9 t
290, V CIS
o 97, R
'kiL 0 J11i .0 ;tj
.4
2

69153
S/i30/59/000/06/009/034
At~, 657110
E032/E114
AUTHOR: FilimonovL-V A.
1-7157"D'e'pth of the Potential Well for a
TITLE: an t e A-Particle in
Eeavy Hypernuclei Ict
PERIODICAL: Izvestiya vysshikh uchebnykh zavedeniyj Fizikaj
1959, Nr 6, pp 61-70 (USSR)
ABSTRACT: The interaction of a &-particle with real nuclei is
looked upon as an interaction with a limited rrtion of
rruclear matter. The nuclear matter is looke upon as a
degenerate Fermi gas and the fact that the interaction
radius for IN.-nucleon systems is small is taken into
G-Ccount. Moreover, the interaction of a A-particle
with nuclear matter in the case of exchange forces is
described with the aid of an effective potential which
depends only on the coordinates of the A-particle.
The depth of this potential well is estimated in the
second and fourth order perturbation theory. It is found
that the depth of the potential well is 20-30 MeV. The
final formula for the depth of the potential well U0
Card J.s given by Eq (39) where B& is the binding energy of
1/2 the A-particle, R is the radius of the residual
nucleus, and the j\,-particle is assumed to be in the

S/139~WAOO/06/009/031+
E032/Ell1+
On the Depth of -the Potential Well for a A-Particle in Heavy
Hypernucle.'L
s
. state.
2here are 1 table and 13 references, of which 7 are
llnglish, 2.1talian and 4 Soviet.
ASSOCIATION: NII pri Tomskom politekhnicheskom Institute
imeni S.M. Kirova
Card 2/2 (Scientific Research Institute at Tomsk Polytechnical
Institute imeni 9_.M-._KFi_ov)
SUBMITTEDi January 19, 1959

24(5Y,21(l)
AUTHOR: Fillmonov, V. A. SOV156-36-5-44176
TITLM On the Depth of the Potential Well forZI.-Partioles in Heavy
Hypernuclei (0 glubine potentaial'noy yamy dlya 11-chnatitsy v
tyazhelykh giper"yadrakh)
PERIODICAL: Zh=nal eksperimentallnoy i teoreticheskoy fiziki)1959,
Vol 36, Er 5, pp 1569-1571 (USSR)
ABSTRACT: In hoavy hypernuclei the motion of LI-particles may be considered
to be a motion in a square potential well the depth of which
depends on the interaction between.A-partiale3 and nucleons. In
previous papers the author, in collaboration with V. A. Lyul'ka
(Refs 3,4), already investigated theA-nucloon potential by means
of the meson theory; the singularities at ishort distances were
eliminated by means of the cutoff method. These potentials
resulted in a regular dependence of the binding energy on the
number of particles in light hypeniuclei. and led to atronger
interaction of the A-nucleon pair in the singlet state. In the
present "Letter to the Mtor* the author endeavors to evaluate
the potential interaction energy of the A-particles in nuclear
matter on the basis of the potential values calculated in the
Card 1/2 earlier Tapers. For the purpose of evaluating potential energy

On the Depth of tbe Potential Well for A-Particlas in
Heavy Hypemuclei
ASSOCIATIM:
SUMUTTM
Card 2/2
SOY/56-36-5-44/76
the nucleons of nuclear matter were considered to be an
incompressible degenerated Fermi gas. Calculations were carried
out for two different values of nuclear density (radii:
and R 2 -1.4 A'1/3.107~13) and are given in a
table. Calculations were carried out for two kinds of K-meson-
baryon bondat acalar and pstudoacalar. The bond between baryons
and pions is assumed to be pseudovectorial (coupling constant
2
f , 0#06). Rectangular cutoff' with kMn 111.js used. The data
were calculated with application of the "iero radius of action"
approximation method. For-10 < A < 20 a well depth of 20 - 30 Mev
'and for A < one of 410 Me-.r '.a obtained; other authors (Ref 6)
obtained 29 38 Mev for heavy hypernuclei-The authir
thanks Professor D. D. Ivanenko for assisting him in this
investigation. There are 1 table and 6 references, 3 of which are
Soviet.
Tomskiy politekhnicheskiy institut (Tomsk Polytechnic rnstitute~
Kovember 15, 1958

24 (5), 21 (7)
AUTHOR: Filimonov, V. A. SOV/56-36-6-54/66
TITLE: On Saturation in the Hyperon System (0 naayshchenii v sisteme
giperonov)
PERIODICAL: Zhurnal ekaperimentallnoy i teoreticheakoy fiziki, 1959,
Vol 36, Nr 6, PP 1941 - 1942 (USSR)
ABSTRACT: One of the characteristic features 'of a nucleon system is the
phenomenon of saturation, which is connected with the nature
of nucleon-nucleon forces (repulsion at small distances, ex-
change character). The forces are first briefly discussed from
the point of view of the meson theory, and the differences in
the forces acting among hyperons are pointed out; though these
forces are of the same magnitude as thoae acting among nucle-
ons, their mechanism is different. Thus, between two A-partic-
lea, forces of second order (exchangia of a n- or a K-meson)
are forbidden on account of the demand for isotopic invariance
in the case of strong interaction. In '11-is ca3e, forces off the
fourth order (exchange of two n- or K-mesons) occiir. The dif-
ference in character of the forces active between hyperons in-
fluences the behavior of systems of a large number of hyperons.
Card 1/3 rhis applies especially to the stability condition. For example,

On Saturation in the Hyperon System SOV/56-36-6-54/66
in the case of systems consisting ofA-partioles and nucleons,
'he stability condition stability with respect to transitions
into the nucleon state) ~1) is: L(m j
'A:m1j', + B(A + L) + TN + TA+
+ U< 0. A and L denote the number of nucleons and A-particles
respectively, the m denote the masses, T - the kinetic energy
of these partiolest B - the absolute value of the binding en-
orgy per nucleon of nuclear mattor, U - -the potential. intor-
action energy of the particles. For the purpose of investigat-
Ing the conditions necessary for satisfying this inequality,
the binding energy of such a system was calculated on the basis
of certain assumptions with respect to the forces acting be-
tween the particles. For this purpose short-range forces of the
Wigner type are assumed between twoA.-hyptarons and between A
and N forces, which lead to zero binding anergy between thp
systemsAAandAN. Repulsion between nucleons is taken into ac-
count only at distances ro a 0-4 f (nucleons and hyperons are
considered to be degenerated Fermi gas). By basinF on these as-
sumptions it was found that in the case of a constant distribu-
Card 2/3 tion density ofA-particles within the sphere with R - r0 L1/3I

On SatUriLtion In the Hyperon 3yptem BOV/-56-36-6-54/66
(1) is satisfied if r 0sw 0.9 f. The particle ratio in found to
amount to A/L f-- 1.6. If (1) is satisfied, the proton.-neutron
state becomes metastable with respect to a transition into the
hyperon-nucleon state. There is 1 reference.
ASSOCIATION: Inatitut yadernoy fiziki I elektroniki i avtomatiki Tomskogo
politekhnicheskogo instituta, (Institute for Nuclear Physics,
Electronics, and Automation of Tomsk Polytechnic Institute)
SUBMITTED: March 5, 1959
1
Card 3/,

M 0',
EIINTING OF PYHR-NUCIE41 ,VD 1'7.-:~tAu S IC-T TYPIXANDkI
E,.D.Ivqnanko,N.N. Kolesnikov, V.A.Lyullka, V.A.Phllirrinnov
H-mervv(_,19, s:-sters containinfl or ~- h-~-)-irons in adriit!nn to -rotons
and mutrnnlif are rif rr.,) t intgrist both 'hr the u- Oirs tand In 7 of cosric -ray
nroc-ins-,~s r.rd for -.~siarcb into orrIl nry nucl-iar forces. By rraiki,:r~ u-9 of t~~e
binr~inrr corstantc ~-nnum "roy- scatterinr, the-r:-, anrl I-avi-Er crirri-3:1 out the "out
of "" fi~ I - tII,- M~ov-HtrtenHus rethod in t)-e U-nry of or.-I 1 nary nucl,~I , we ob-
ta-rprl -.-ili ~? f-r h ,--3r-nucl.91 bindin:, ener:-i-s ir q-iti!7factory wit!,
Oxn--r 1 rent-- 1 r7l'-, I I V- .
An iviNatinn radp on tl,q b-inis of Nold ti-iory riv-1,34 t~-~ -t~x:Irt~)ncq of
wa-~ rr-.rc3!- of A-k att,raction in -:ridiVori t~i --~rev perm ~ TI, t,3 re : ct ion,
wH!.ch, in turn, is nnt.',Y3 bly vi kir than t~,3VN forcer, . Tn tI!,.s conn-3ction,
ti- ~ b;i1(P,)r- eiv)r-`~?s of tl,i n-rmal and t~- r3-1,cito-i -,t-.'13s ~` a of light
-ucii; cont.-iin-'rg rnp_ or twnA- narticlos .P-r,3 Cq] C 1 7.,~ t(- rl vEl;n!~ V,a
annroxiration of i slort ranF;~ rf action cArid a -otontial denarding
on t~j 5,jr I _P "araretirs i-mro, selecte-I m as o 1 r,"vr,:i Vo -nc ~s-ary b, ndi! f,
onorrry of t'r?" n -Ind
TI- i~itsi on f or c--~ s-r-c-_i-)dI.-.!, fror NA--r--, ern'_-,ye-4~ to
calculate t~i c-os!7 s--3-ction oil scattarit~p~id cantu-e s2owj~_
n9rticltis ty nucl,-1.
Rq ~orf. , r-i-intil at V,3 In"r-aVonal Conric Ray Confore- ce, Mo-cow, 6-11 July l')5T .

21(1)t?1(7) S 66
AUTHORS: Ivanenko, D. D., Lyu.11ka, V. A.,
TITLE: The Theory of Hyper-nuclei (Tooriya giperyader)
PERIODICALt Uspokhi f i z i ohe skikh -nauk p 195 9, Vo 1 69 p Nr 4, pp 6
ABSTRACT: The authors give a survey of the preqa_nt stagi. of -6ht: "h,;-
hyper-nuclei, nuclear systems consietilig of nuol,,~ons aad
hyperons. An investigation of these lh;'per-nuclei irakes it
posvible to obtain data on elpmortary partioles (A.1"Eq Y
such as spint parity, and the interaction between partiole--;.
The large amount of experimental material available in tli!-
respect makes it possible to der~l in thecry mi-th hyrer-1'11c1.--;,i_
toth from the phenomenological point o.~ viewt and by mertns
the quantum field theory. The authors enixiierate th~ mos'~
essential experimental factoro Pnl fhe maost import'r-it,
theoretical investigations concerning hyperons. The experimental
part of the paper begins with the-discovery of hypernuclei in
1953 by the Polish physicists Danyst and Pniewsky (Ref 1) in
nuclear emulsions (Fig 1); in the following, the authors disclieB
the :Identification of hyper-nuclei; a table shows a numbaz~ of
Card 113 hypernucleue observations. It was found that whereas in the

The Theory of Hypor-nuclei
SOV/53-68-4-4/12
case of accelerator- and cosmic radiation experiments, the
relative frequency with which hyper-nuclei are recorded is
about 1.10-3 (cosmic rays only 0.2,10-3), it was found to be
between 24 and 57-10-3 for the ease of K-captures. In the
following the question of the life time of hyper-nuclei is
briefly discussed; their value is near the order of magnitude
of 10- 10 sec. Furtherg the frequency of hyper-nuclei as a
function of the nuclear charge is discussed. Figures 3 and 4
show the Z-dependenoe of mesonio ana non-mesonic decay.
Finally, the binding energy of the Apparticles in the hyper-
nuclei in discussed according to ihe relation
B - M + M - 1: mi - Q (Figure 5 shows B (A) - a straight
A A -A L A
line; A denotes the number of nucleons in the hypernucleus,
mi the masses of the reaction products, and Q - the sum of their
kinetic energies), and also some anomalous cases observed. In
the second part of the paper - the theoretical treatment of the
hypernucleus problem - the most important properties of the
hyperons and K-meeons are discussed (classification of inter-
Card 2/3 actioft into strong, electromagnetic and weak interaction, the

The Theory of Hyper-nuolei SOV/53-68-4-1/12
theory of the formert special cases, some and Z(-'processej,
after which the decay possibilities of hyper-nucle.1 mosonio
and nonmesonio decay), as well as the problem of the spin of the
A-particles. In the following, the authors first ment~ion 30me
general questions of a phenomenological treatment of the hy or-
nuclei with A 4 5P followed by the special cases of' the hyper-
nuclei He5 H4 H04 and H3 . Finally, the treatment of
A I ~h- I ~& :6.
light hyper-nuclei on the basis of the field theory anet
questions related to the spins of the hyper-nuclei are
discussed, The material (particularly that of the theoreUcal
part) was mainly taken from Western papers. There are 5 figuxes,
5 tables, and 136 references, 12 of which are Soviet.
Card 3/3

694-36
S/139/60/00o/ol/olo/o4l
E032/E414
AUTHOR2 .,Filimonov, V.A.
-----------
TITLEt -b-n-the Binding Energy of a System of Nucleons and
Hyperons
PERIODICAL: Izvestiya vysshikh uchebnykh zavedeniy, Fizikaq
196o, Nr 1, pp 6o-.63 (USSR)
ABSTRACT. Recent work has shown that the hyperon-nucleon. force
is attractive and is of the same order of magnitude as
the nucleon-nucleon force. One of the characteristic
properties of nucleon-nucleon forces is the so-called
saturation phenomenon. Various suggestions and models
have been put forward to explain this property. For
example. the saturation of nucleon-nucleon forces has
been ascribed to a repulsive hard core (Ref 5), to many-
body forces (Ref 4) and to the exchange character of
the forces. The general view at the present time is
that the saturation is a consequence of the presence of
a repulsive hard core and the exchange part in the
maucleon-nucleon potential (Ref 6). The basic features
of nucleon-nucleon forces can be -,-)btained from the meson
Card 1/5 theory in which the repulsion at small distances is

MI
6%)43t
5/13q/6o/ooo/ol/oio/o4l
E032/E4i4
On the Binding Energy of a System of Nucleons and Hyperons
Associated with the existence of the function. 6(r)
in the second order.potential of the pseudoscalar meson
theory. This point of view if; confirmed by the
interaction of nucleons with antinucleons, If this
view is accepted then in many hyperon-hyperon and
hyperon-nucleon interactions one would expect to find
forces without a repulsive core. This would occur in
the absence of an interaction associated with single
meson exchange, the meson interacting pseudoscalarly
with barions. An example of such an interaction is
the interaction between two & particles in which
second order forces are forbidden by the isotopic in-
variance of strong interactions. The absence of
repulsion at small distances will lead to a considerable
difference between a bound system of a large number of
.A particles and a nucleon system. In particular5 one
would expect a large mass defect in the former case.
This would ensure the stability of the system against
a transition into a nucleon state. It is shown in the
Card 2/5 present paper that the condition for the stability of

69436
5/139/60/000/01/010/041
E032/E414
On the Binding Energy of a System of Nucleons and Hyperons
hyperon systems against transition to a nucleon
state may be satisfied for densities comparable with
the densities of nuclear matter, This means that one
can use methods employed in studying the properties of
nuclear matter in the discussion of systems containing
hyperon5. The mass of a system of interacting particles
is given by Eq(l) where MN and m,.%. are the masses
of nucleons and -4 particles respectively, and A and
L are their numbers; TN and TA are the corresponding
kinetic energies and UN and ~A and UAN are the
potential energies. If the nucleons are looked -upon as
Fermi gas, distributed with a constant density in a
sphere having a radius RA = rAAI/3, and the
A particles in a sphere of radius
RL = rtLI/3
then the k:1netic energies are given by Eq (2) and (3)
where r,7T and MIT are the Compton wavelength and the
mass of -TT mesons. In order to calculate the potential
energies, it is assumed that the hyperon-hyper-on and
Card 3/5 hyperon-nucleon forces are Wiegner forces of the Yukawa

69436
S/139/6o/ooo/oi/oio/o4l
E032/E414
On the Binding Energy of a System of Nucleons and Hyperons
type, having a radius of action equal to one half of
the Compton wavelength of a meson (cf Eq (4)) .
The quantity g2 is chosen to be of the order of 0-5-
The potential energies are then found to be given by
Eq (6) and (7) (Pauli principle being neglected). If
one assumes that the radius of the hard core for
nucleon-nucleon interactions is of the order of 0.4 f,
then UN is given by Eq (8). The binding energy of
the system is defined as that necessary to transform
the isystem under consideration into an aggregate of'
non-interacting nucleons. The binding energy per
particle is then given by Eq (9). Tile condition for
the stability of the system of nucleons and Aparticles
against a transition to a nucleon state is E> 0,
provided one neglects the binding energy of nucleons in
nucloar matter. The ratio of number of nucleons to the
number of A particles which correspond to a maximum
binding energy can then be found from the condition
Card 4/5 given by Eq (11). Table 1 gives the binding energy for
aia_~ ~11

69436
S/139/60/000/01/010/041
E032/E4i4
On the Binding Energy of a System o-f' Nucleons and Hynerons
two values of g2, namely 0.5 and 0.25~ As can be
seen from this table, the stability condition is
satisfied for g2 = 0.5 if 0. 9 2 f If g2 = 0.25
the condition is satisfied if r o.64 f These
quantities are to be compared wit~rN = 1.2 f which
characterizes the density of nucleons in nuclear matter.
There are 1 table and 8 references, 3 of which are
Soviet (1 translation from English), 4 English and
1 Italian.
ASSOCIATION: NII pri Tomskom politekhnicheskom institute imeni
S.M.Kirova (Scientific Research Institute of the
Tomsk Polytechnical Institute imeni S~M.Kirov)
SUBMITTED: March 28, 1959
Card 5/5

S/139/6o/000/004/027/03:5
E032/E514
AUTHOR: Filimonov...- Y:-A-
TITLE: The Role of Three-Particle Forces in the Interaction of
a A -Particle with Nucleons
PERIODICAL: Izvestiya vyssAkh uchebnykh zavedeniy, Fizika,
1960, No.4, pp. 222-228
TEXT! Meson theory is used to obtain 3-particle -&-nuclogn
potential. The 3-particle forces are due to the meson exchange
between three heavy particles. The simplest 3-particle forces
correspond to the two-meson exchange. In order to calculate the
3-particle potential, use is made of the nonrelativistic Hamiltonian
for the interaction between fixed baryons and -W - and K-meson fields.
(these are given by Eqs.1-3)- An expression is derived for the
potential energy of' the -& -particle in nuclear matter. The energy
turns out to be negligible compared with energy due to pair forces.
There are 1 figure and 11 references: 5 Soviet and 6 English.
ASSOCIATION: NII pri Tomskom politekhnicheskom institute imeni
S. M. Kirova (Scientific Research Institute of the
Tomsk Polytechnical Institute im;-"-1 S.
8UBMIT~f:D: September 14, 1959
19

FILIMONOV, V. A., Cand Phys-Yath Sci "Ilypernuclei and
the interaction W A-hyperons Wilk-nucleons." Mos, 1961.
(M!.n of Ed RSPSR. Moo Oblast Ped Inst Im N. K. Krupskaya)
(KIj, 8-61, 229)
53

FILD40NOV VIA*; 11AxOV61UY, V.Ye.
Exother=l and endothermal roactions in the decompostion of peat
[with summary in English). Inzh.-fiz.'zhur. 4 no-3:18-25 Mr 161.
(MIRA 14:8)
1. EnergatichesIdy institut im. G.M. Krzhizhanovskogo AN SSSR
i Kalininskiy torfyanoy institut, g. Mcskva.
(Chemical reaction, Heat of) (Peat)