SCIENTIFIC ABSTRACT MOROZOV, YE. M. - MOROZOV, YU. I.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001135230001-5
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: July 13, 2001
• Sequence Number: 1
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

FRID14kN, Ya.B., prof., doktnr tokhn.Tiauk; IAOROZOV, Ye.M.. kand.telchn.
nauk r ---
Calculating mechanical properties of bimetals. Yauch.dnkl.v7s.
shkoly: mashA prib. no.1:1~?-Ih3 ' 58. (MIRA 12:1)
1. Predstavleno kafedroy "SODrotivleni3re materialov" Hoskovskogo
inzhenerno-fizichoskogo instituta.
I (Laminated metals)

,%CROZOV. Ye.M.. kand.tekhn.nauk; FRM-LkN, Ya.B., doktor tnkhn.nauk
-
Palculatinp, the 1)ri~tln-breakdovr resistance of a disk stretched
In all diroctionn. 1Taur1n.dnkl.v79.shkoly: mash.i prib. no.2:
"'9-12 '58. (MIRA 12.'10)
1. ProdstRvlonf) kaffidroy "Soprotivlnnlyn naterialov" Moskovs'koro
1nzbevo%rnn-fizichps1cogo instituta.
(Strength of materials)

FRIDHA,N. Ta.b.; MOROZOV, Ta.M.
Approximate-evaluatlem of concintrated stresses in comocite
specimone. Nauch.dnkl.v-,-s.ohknT7; mash.l prib. nn.4:r?,2-F,5
I f.
,9. (MIRA 12:5)
1. Statlya predstav-lena Monkovskim lnzhonerno-flzichoqkim
Institutnm.
(Strains ai.1 stresses)

MOROZOV. Ye.14., kand.tekhn.nauk
Choice of the thickness of the liardened la7er of engine piston
rings. Trakt. i sellkliozmash. no.5:45-47 M7 '58. (MIRA 11:6)
(Piston rings)

j02

- /6-
'
~27
2 2 1
A _j 61'1'1 1,:orozov, Y e
t e C) f
C C,_~
TI-1-j-.ol: On tl~t~ est 4 m-, io n of -2- i.. I r,(--
t i 1 0 e C n j k i r,
I,-- v L:3 t i y a vSr3h _'~:il uci!qhnykh z;tv,2~eniy. L:: n
stroyeniye, no. 1j, -960, 5'~ - 61
-L'X-: The articLe 4orms an at on ~_n,_` Ytic,,! let, n 'ion of
+ s ~_ r e s :; e S t e s~ C. C 0 4
..-Ln-,! ; in
s aL3.-i med to two r~X,2s of s:!7=e-~ry ,
_niso-
t.-,,--,ic coe'--ic-ents of 1;nuar e x -a r s as e
-,n a a n'! a
'ic !.:() itil L iLlld D, 1 1
.-rains are Jeformed tot-ether, oil-dnt- to exp,-.nsion, urd' ti~,_.refore,
4
nor,-ra-l and tanEent stresses are ,-roduce,.~. The lr.~ent-t.;r,!. _I-rain
bo-,~ndf_='es results in s.,lift of elementuary volumes alor_,.-_ '11--]-se li-
ni~;s. --ne deviation of crain bc),.,n-- ry S frr~,% -* tp 4 ni ~ :,,,7 '.-'r)n
i~- L-iver. by
C,~,~r-i 1/3

o2 3

r o
22..
10

r
9 of for 'vir. .,ic.-?nt n

14 IA -30
d by ~r.~Vlo!Z.-.1y by ..2 an'
:- J). 'fo evaluate the aut"J"r
ii . ,-er of llpl::"~,rature cyt, I,- -'rid, I-Iii,i,3, ri f
'ht-. second orlr~,r urior to ti,,~ Of cr,,~C~S 4~;
K

(Y _ ,,)n
fE, tiu pi;..jtic zi:x,%.,, per ono
t
-,,tion a. tnt.,
e f o I

--I of sperimen. "i. rau*L(-Ir ',tekej t_ i-s ar. ,L,,b-*- t-, r- tu-
e
4 1, no _S 4 vi' c. -
+ W, C 1, C"aCl
. . Ce fur.,~:e~ e n u n _m ,D

-r d 2/3

n.K r
--re arc. s
ar-, d m r) r-ji
9 .9owev r
ELn
er
rill a W
L r. C T
e r
S 31M 1 TF D .

MOROZCV,--YeaM.p kand.takhn.nauk
Approximate calculation of thermal plastic atresses
Izvevys*uoheb*zav.j mashinostr. no.g:U-18 161 ~141RA
in a pipe.
1-4:12)
1. Moakovskiy inzhenerno-fizicheakiy institut.
kIThermal stresses)

6' /,) 1 C/,~o o/c. 0 -1 /0 -
ks
1,1TEOR3 I Friimhr. . Ya. Z,- SoDoloy, N. D. , Borisov, S. V. To,7-.Y-,v
.7 Kono~ snko , 7 ro-ov , Yo. M. Saa-:5va. 0 v ,
h, Snorr, 5. J'.
TITL!Ci Soizu pr,)olocs of thermal atren6th In reactor cunatzi;ctlan
PE.iIODICAL, Atommaya on,,rgiya, Y. 1-0, no. ~, lt~6i, 6G6 - 6!9
7 SX~ I Tn'd llia Of Of tliGrMal Eilrvn,~,h inc:.Ui,~G two
zyp~B of frac*-.r4l ti,o jr,!ua, (a-uccrtical~ fracturi as c--,5a-,U(,nCu
o~ an eitrume d~f,)rmatior, or o' a j"reat of aracka 1 i:*C-~-aized
truc?2; ca-uiv3 d.A m.nlfuGLa,.-or5 Of *.n-,:;o :,Ucturoa are
tn a I j o f t !c ~, r c a t ro n gtn. on -.I-. ae 3,1C;0 -.I,.
',y;;j Of frac.uro maj be brought tj four
Of s' zjc*l&r.Ice..' Or L".o.-ma. sho~:k stresioal 2 , brief 6LLLt Ic loula
for tc zr.~,nutuj or nour:;; - , :;-~a' ',:~ loada for soma montlia or years; 4 ,
P.-j'-UntG glumplea lln the variatior of elalt' a and
pii c3nd, tions !,-. a ti'--o , a:-.~ a fictitioue o'jaStlo tonalon !a ohovn
A 'darzod 1 Ino' , vhl~e the forms of mechanical
Lo arl.u Iln tra p' abtl~; zone
Card -./X~

-G Ozza th rz., u t
an! "~..rn" in ,,rc-O",
U--.~.Our as a rf
a', r- )i ~a:c,.at,,n,~ *.:,,u croup1r.. .:).-OCUa3 thd
a of crac-P th.)ury that tr~orc to a ,~nticna~
uutwQan tnj rat.) of roap v, , the r) j.'.
,h. tarapjcatura T, thd I me T ftni '...a pla3tle d4fon)atior. P. num""Y'
H u ru, T' P. The
-VI
an a -
a r z, r r a a a' .1
L~S~.,Or, tra frac'.t;re ajpuara '.r(sady aftor !V-10~ cyc:fj
7 5
lak.4-,, 10 -IG cyclo- ta ap?.ar. A
af*.~-,.~.a,--ai frL-tur, IQ tn4 Iaza', doforz~,,tlon In zonos EL r
Lu=~urataro diffor6ncQ allao in hozQ,,:unuous ftaldu a' 2*1.ro~u~ T 1~ f,
a
.,a--; to tmi appaLr;,nno of hiCh
I I ~Tzblo 1
tno-zall e~-.ockti Lri% tempcratarfs ~Iuzp giving r1ae to u briltls) frLct"Iro Mal
Card 2/Xi

)71.0
so=. pro,-.10=3 of tlne~-~.al Strenrt- 3-50 k-C-1
'-0 o3t!=Utd! by an eq*.;'.'I~~'-.. ~f In t'-e ~ract'--O' ts
the creeD c-aracter rn. .i of 7n-n'e:--a-
m-~:hanlca' and nonstealy are
strated in F4g. t c-~rv,.3 o' varlat lon of
'sca'~ 4NiO or,- cycll~: t')Z~erature tno
t--.] r=a' an! oln.3 tic efo r-.at4 on A a o t 0 c 0 ztn 5 3 C D
e --9 ', -e 3: CFa:*F~Ct-2~-L3.!1 C~)nCvTn-~! 15
o ns n c s '. z' a'- n
increased te=-'e~-aturea, in of a :~-~-Ply zt:--s
ara of' a thermLL. ori~7'.n a:.d 'oa! tD of bt:-'jc".ura'- olemrjn6.!~ In *.',.o
hot zones, w'.tnout., h~reve:', ca--3~r.K~ broaKdown. The m'crommec'-a-lc-
a: properties w.3re c- -ockel n t7;o ways. The principlo of the se':on~~ is
illustl-atod in Fig. 15, whl~e tllne raoult8 of the former - for static
olong,attons and at 1403 - 15COoC in vacuum or in a controlled- atmosphere,
are prosonted in Fig. 12. :n -ip,. 13, 1 denotes the aamplo a cross
sect' on of 2 or =m' at Is placed in a groove milled out from
block 2. The prossure is yioldef! by staz:;) 3 =ado of tungsten briquettes
4. The resulting breakdorn is Indicated over co-ntact 7. There are 13
figures, 5 tables, and 59 reforencest 27 Soviet-bloc and 12 non-Soviet-
11'oc. The three most recent references to Englisb-languago publications
Card

55me Prob"emi of c -
rer,A as --o' Ion at 'bract-. r i York , 71. ny an Cor. r n'-- 0 r7
',a 'k rav or ty p th. 2: 5 19- Ot
.. ar'~. 17 no - 2
C
a'. J. Inst. Meta'-,, ~:ay
7 -.:) ISoptom"Or 19 1960
-------------
Lc,and to Fif,. 1, Di3trIlTation
of the pla3tic zone in a thick-
walled tube with various to,-.,-,Draturo
Jumps: r - radius of an arbitrary
point; a - imner radius
C a rd 415~\ ~-i

1116TWZOV, Ye.M. ; FRIDMA1.1, Ya.B.
Trajectories of cracks of brittle fracture as geocetic iir,~~,s cn
1 11
the surface of bodies. Dokl. ~N SSSR 139 no.l:F7-90 Jl 161.
(XIRA 14:'~')
1. Predotavleno akademikom G.V. Kurdyumovyni.
(Strairw and stresses) (,,"lasticity)

e5, 0-;j
85
te
Ae

44/:JC,2/r) 15/026
'n io- of
YLL
:j. t:.e
r
h
t
'-,,-or- tion. pne
V, j ! f the n e t r i c
In t"lis
If tne
f 0 The
10 pmen t
Grac", dovel
r ~L,:: :.cide:~ --,kith a geodetic
6

'aces 'orm during
2--~-y2 y'3 dx 0
Y) 2T rx
L
f r I If 1 9 ~--9 Zhurn
,ec e.-. f, L::-. 3 V
.,ca ;e'-.ician

AP4038521
S/002o/64/156/003/0537/05110
yo, ~1,; Folaky Ya'
in f3olido
I I IC tjd(~'; 0 cruck
P171
7 - 13 Cil

C "'L
a -1 Li t
s U:~,a
'D

L 065~-,,-67 L )/F,,
ACC NR, AP6029856 SOURCE CODE: UR/0032/66/032/008/0977/0984
~ALTI'HOR: Morozov, Ye. M. Fridman, Ya. B.
i,)RG: Moscow Engineering-Physics Institute (Moskovskiy inzhenerno-fizicheskiy institut),
t!T'~E: Crack analysis as a method of determining fracture characteristics
SOURCE: Zavodskayd laboratoriya, v. 32, no. 8, 1966, 977-9811
TOPIC TAGS: material fracture, elasticity tneory, crack propagation, thermodynamic ana-
iys.-*Ls, variational calculus, approximation method
A i3 S TRA C-1 :The variational principle of crack anaiysis based on rLialiratilive experiment-
I
ai and analytical techniques was used to study causes of fracture. Mechanical and ther-
modynamic methods were employed in determining crack trajec.tories and their mode of
propagation. The functional
E - L,js
was related to both equilibrium, (6E 0) and nonequilibrium cracks 8 F d f0.
vihcre E is the difference between the energy absorbed J Y dS and supplied F dS to
either type of crack. Since cracks form in zones of maximum energy absorption (stress
UDC: 620.17
Card-1/2

I. 065~3-67
ACC NRi AP6029856
concentrators), different stress concentrating states were analyzed. Eleven conditions
ar,~! given whereby cracks terminate or propagate along preferred plaries or d1rections.
The fracture toughness (KC) was related to an experimental modulus of cohesion CK).
,,odifications of the Griffith theor-j were made in order to include the effect of a,,
the largest value of stress occurring at the ends of a crack. Approximate variational
methods of determining crack trajectories are Vven and experimentally confirmed on
samples with a circular stress concentration.- Another approximate technique, the meth-
od of cross sections, was used to analyze ellipsoidal notches of various lengths lying
at different angles to the principal stress direction. The calculated critical stress,
given as a function of crack angle, showed the largest deviation frm exact values at
.lower angles (below 300). This method was also applied to the case of two adjacent el-
lipsoidal notches, and the dependence of the cc--'culated critical stress on the ratio
a/Z was presented for crack propagation on both ends of the cracks. Here, a was the
distance between the cracks and I was the crack length. Orig. art. has: 5 figures
f :19 formulas.
suB com: suBm DATr,: none/ ORIG REF: 011/ OTH REF: 004
Card 2/2
T_

MOROZOV, Ye.M., iazh.
Interchangeable equipment for the M-151 excavator for
digf-;ing trenchas in frnz~in ground. Strci.i ior.ma3hinostr.
4 no.12:9 D i-59. (MIRA 13:3)
(Excavating macbinery-Fiquipment and supplies)

IZMM, I., kand.telch.nauk; KGROZOV, Te.H., inzho; 'ITKOVSKAYA. T.T., inzh.
Interchangeable equipment for ETU-353 excavators for digging canals
with trapezoidal sections. Stroi. i dor. mashLuostr- 5 no.8:14-16
Ag 16o. (MIRA 1-3:8)
(Excavating machinery-Equipment and supplies)

Aob,.',(
for 4cr'.,:'L- ro.-
:14-16 l6a.
14
(EXC aV~ t 4 n '.-;r. r -y)
,L
(Frc -- cn .-r-

".,C' , A.A. k
"AVIEL "Y ~ A' I'L - C 7. A,
Chain and '-Uck(- 4 rei;cl.ir.,- 2--:c:,vatc.-: e; n- E, t ra r, Le
Lv w. o i-.- . o. kv
rench i..--t:in;

q-t-.',th ary-'- the.
t4riAtijid:,: liv OMS Jit -~Ehd :k
-,id .-d
e-cons ert ':as
,C'. toms a'
u ts e- r

SOSINISKIY, K)11,70110 Y#-.N.
Occurrence of negative a,,~sorption In a portion of a lo--,-_-er-
4 spektr. 18 no . - X- '~5-
broadened line. Cpt. 3:510 512 -
It )
. ~I --A --R: r,

-_ 'Ili "buzWob SOURCE CODE: UR/0051/65/019[00470_6_3W6_G35
AUTHOR: Sosinskiv, M. L.; Morozov, Ye. N.
ORG_ none
TITLE: Luminescence and absorption associated with the lower terms of cobaltous
and nickelous ions in ZnS single crystals
SOURCE: Optika I spektroskopiya, v. 19, no. 4, 1965, 634-635
TOPIC TAGS: zinc sulfide, cobalt, nickel, luminescence spectrum, absorption spectrum,
spectralline
ABSTRACT: ZnS-Co and ZnS-Ni single crystals of the wurtzite modification with an
activator content of 0.5 to 0. 005% (in the initial mixture) were grown by the Bridgman meth(
and their absorption and luminescence spectra were measured at 10, 20, and 77K (Zns-Co)
and 4.2K (ZnS-Ni). Fig. I shows a schematic absorption spectrum associated with the
excitation of the lower term of N12+ ion in Znq. The spectrum contains three narrow bands
with frequencies of 4386, 4374, and 4277 em . and several broad bands which may be due
to electronic-vibrational transitions. No luminescence of N12+ could be observed in ZnS.
The position of the terms to described by the crystal field theory for reasonable values of th
field strength Dq and Racah parameters B and C. The theoretical schemes of the two lower
terms of configurations d7 (Co) and d8 (Ni), allowing for spin-orbital interaction, are given.
The number of lines observed in the absorption spectrum corresponds to the number
Card
UDC: 535.370

ACC NRt AP5025306
Fig. 1. Absorption spectrum
of ZnS-Ni crystal at T4.2K.
A,jiAiF
r, I fa a /I
1, I-VI /A 1)
~jl
1.18 Z14 A "Wo
expected from this scheme (if it is assumed that the broader bands in the spectra of ZnS-Ni
crystals are associated with the appearance of phonons). However, no definite comparison
between the observed spectral intervals and the structure of the terms 3T2 could be made
for Nj2+ ion and 4T2 for C02+ ion. Authors express their thanks to M. B. Yepifanov for
assistance in the construction of the measuring apparatus. Orig. a7r-R-as- 3 figures.
SUB CODE: 20 / SUBM DATE: 16Dec64 / ORIG REW: 005 / OTH REF: 003
-'~~2 / 2

1 ACC-NR, ~p6o36964 C,5-,Ar) SOURCE CODEs di[0181/66/0-08'/01-1/32-36-/32-40,
A71'HORC Alferov, Zh. I.; Garbuzov, D. Z.; Morozov, Ye. P.
ORG3 Physicotechnical Institute im. A. F. loffe, kN SSSR, Laningrad (Fiziko-tekhni-
chaskiy Institut AN SSSR)
TITLEt Effect of heat treatment on the photoluminesconce of gallium arsenide
SOURCEI Fizika tvordogo tola, v. 8, no. 11, 1966, 3236-3240
TOPIC TAGSS gal-lium arsenide, photoluminesconce, recombination radiation
ABSTRACT: The effect of heat treatment of n-typo and cadmium-doped p-type gallium
arsenide on its photoluminescence spectra was studied. The samples were heated for
3 hr at 270, 370, 450, 520, 580, 710 and 8801C, and the spectra were recorded at 77
and 300*K. It was found that the position and intensity of the longwave bands of re-
combination radiation are determined by the con(iitions of heat treatment of the crys-
tal. When the latter Is heated in quartz ampoulo3 above 70011C, the fraction of radi-
ative recombination decreases sharply, and the entire radiation falls w-ithin the nar-
row band of 1.35 ev.
Radiation in this band is due to the recombination of excess
carriers ac--oss one of the acceptor levels of copper. Heat treatment at lower tem-
Deratures (450-6000C) causes a strong luminescence in the 1.2B-1-30 eV range and a
displacement of the 0.96 eV band in the initial material to an energy of 1.01 eV.
These changes are attributed to the introduction of lattice defects during heating in
L C.,d 1/2

ACC NRi AP6036964
the presence of copper. In conclusion, authors are grateful to V. M. Tuchkovich and
D. N. Nasledov for their constant interest and attention to this work, A. N. Yermakova,'
for assistance in the experiments, and D. N. Tretlyakov for a number of useful sugges-I
tions. Orig. art. hast 4 figures.
SUB CODES 20/ suBm ans 09Apr,66/ ORIG REFS 004/ OTH REFS 007
2/2

MOROZOV, Ye. V. -
"A Study of the llectrode Processes Durir~-, the Electrolysis of Moncyanite
Solutions of Zinc and Nickel." Cand T.9ch Sci, Moscow Order of Ien!n Chemico-
technological Inst iment D. 1. Hendeleyev 27 Oct 54. (TM, 13 Oct 90
Survery of Scientific and Technic,~Ll DiFi3ertati-me Defended at USSR Higher
Educational Institutions (10)
SO: Sim. No. 481. 5 May 55

/Vj 0 J-j 6 L Cl V, )14-. 1/,
IZGARYSHEV, N.A.; KUDRYAVTSEV, N.T.; KOROZOV, Yej.
1.
Production of shiny nickel deposition from ammonium electrolytes. Dokl.
AN SM 96 no.1:14)-144' Ky 154. (KLRA 7:5)
1. Chlen-korreapondent Ak-ademli nauk SSSR (for Izgaryshev).
(Electroplating)

MOROZQV2___jx~A.; RYBINSKIY, D.A.
New carburetor of the "Volga" automobile. -.v-t.prom. 27 no.lC:
9-3.1 0 161. (MIRA 14:10)
1. Gorlkovskiy avtozavod.
(n'utGmobiles--Engines-Carburetors ,i

RYBINSKIY, Dmitriy Alekseyevich; kl-OE9-ZOVI Yur4 Al!j~r~q* GUTKII,
Samuil Grigortyevich; KONEV, B.F., inzh., retsenzent; STROKINA,
T.I., red.; WAROVA, A.F., tek-hn. red.
[Caburetors of the GAZ engines] Karbiuratory dvigatelei GAZ. Moskva,
Mashgiz, 1962. 254 p. (MIRA 15:7)
(Automobiles-Engines-Carburetors)

PXKHOV, I.S., inzh.; MOROZOV, Tu.A., inzh.
Interference caused by an inductive signal 'In consolidated networks.
Avtom. telem. i aviaz' 3 no.8:29-30 Ag '59. (MIU 13:2)
1.11auchno-issladovatellskaya laboratoriya Novosibirskogo
elaktrotakhnichaskogo instituta svyazi (for Morozov).
(Coaxial cables) (Electric transformers)

SAVYIN, M.M.; MOROZOV, Yu.A.
Investigations into the causes and nature of electrical troubles
in contact networks in mi-nes. Trudy Inst. gor. dela Sib. otd.
I
AN SSSR no.3:240-251 160. OMI'LA 14:4)
(Electricity in mining)

MOTIOZOV, Tu.A.
lweBtigating high-frequency interference in contact and power
nntworka of minpa. Izv. Si b. o tj A)j SSSR no. . : 42-50 16 'j.
(MIRA 13:7)
1. Novosibirskiy elektrotekhnichei3kiy institut svyazi i Institut
gornogo dela 6i'-Arskogo otdeleniya AX SSSR.
(Electricity in mininr,)
(Remote control)

MOROZOV, Yu. A.
Cand Tech Sci - ( diss ) ".-,tuly of e' ectrical di sturib.-nces ~ r' -,; r'-
.; 4V
tact networks of mines." Moscow, 1961. 18 pp; (Inst off MirAn '
Affairs imeni A. A. Skochinskiy); 2(,,0 copies; price not given;
(KL, 10-61 sup, 216)

I-IGROZOV, Yu.A.
High-frequency oscillations and their dam-ping in a mercury rectifier
0
network v1',h ground equalizer. Sbor. rab. po vop. e'ektromekh.
no.5:262-275 161. (MIRA 14:6)
(Electric currert rectifiers)

SIDFILINIKOV, V.V.; MOROZOV, N.A.
Use of power networks for the transmission of information. Vest.
AN SSSR 31 no.6:99-100 Je '61. (MIRA 14:6)
(Telecommunication) (Electric lines)

MOROZOV, Yu.A.
Interference generated by the nonlinear elements of electric
power distribution networks. Sbor.rab.po vop.elektromekh.
no.7022-326 162. (MIRA 161l)
(Electric lines--Overhead) (Telecommunication)

MORO ZOV, Yu._A,.- -
Use of the contact network of electrified railroads for high-
frequency teAlAommmications. Sbor.rab.po vop.elektromekh.
no.7:326-330 162. (KERA 16:1)
(Electric railroads--Wires and wiring) (Telecommunication)

V
7!1 - 4 12 3
AUTHORS: Shul'man, A.R., Zakirova, I.R., Miorozov
Fridrikhov, S.A. 1.i.A. anJ
TITIE: The Problem of tte Metl~od of Investi~,atioi_ of Secondar-.
Electron Emission of Non-metallic SubsLances (K vo-'rosu
o metode issledoverii.,/a vtorichnoy el,?ktror,.,oy
nemetallicheskikh veshchestv)
PERIODICAL: Radioteklhnika ' Elektronika, 12158, VA. III, No.`
Pp. 329 (USSR).
ABSTRACT. Description of a me~!.od of the me,, sure me- 15 of secoid,:.i-_,,
electron emission is L,4k-ven. The method is chriacterised !~y
the following features: reduction in the time necessary for
the experiments, increased accuracy, good stab--'Lity of the
measuring system and the target anic eliminatio.L Of the terris7l-y
electrons. The Fiain coj,~ponent of the experimental eauinment
used in the measurements is a spherical, glass bulb
fitted with apertures for a target and an electron gun. bia-
meter of the sphere is 145 mm. The electron .7in is of the
standard type and is provided with a focusinE Plectrode; it
is also furnished with a reflecting diaphragm wl-ich eliminates
t',--e scattered electrons fro-- the bear. of the (~an. The dia-
phragm is given a Dotential near to t1lat of the cathode. "lie
C~,rdl/4 gun is screened by means of a nickel cylinder. The target iE3

I W-1- 3-4/23
The Problem of the MetLod of Investigat'Lori )f Secondiry Elr~ctrjii
Emission of non-metallic Substances
C-~-rdZ/4
in the form of a round, flat box '~av-r.F a dlazetc-r of 1~'~
and is fitted with a helical heater. The target is fixed on
to molybdenum supports and provided with a pair of leads for
supplying the current to the heater. The heater can be earthed.
The supporting wires of the target are taken to the input of
an amplifier. The effect of ternary electrons is reduced by
placing a spherical molybdenum grid, havinE. a diameter of
125 min, between the collector and the target. The transparency
of the grid is of the order of 0.9. The grid I-as an aperture
with a diameter of 40 mm for the leads of the target; another
aperture, having a diameter of 16 mm, is provided for the
primary electron beams (impinging on the target). Both the
glass sphere and the grid are coated with silver by means of
an evaporation process carried out in vacuum. For the analysis
of secondary electron energies, a de-celeratin-F potential
U3is applied betneen the target and the Erid; a potential
U9 is applied between the grid and the collector, w.Jch
accelerates the secondary electrons and SlOW3 down the t~.-rna
ones. The full experimental equipment (which was built around
the spherical condenser) is shown in FiC-1. This consists of

The Problem of the Method of Investigation of Second--iry Elect--,,n
Emission of Von-metallic Substances
the above mentioned electron pin, the ccllector and the a-+I--i-
dynatron grid and contains the followini, units: supplies for
the electron gur-,. a rotary potentiom~eter,.su,-_i~iies for the
potentiometer, 9 sync1ironous motor' a reE:isterin~ instrument,
~ delay circuit, a r,_~ctangular pul'se genprator, -an amnlifier,
~ pulse lengthener%, an oscillogrraph with a tri.--r..,!~edtime base;
an automatic switchiriE device and a synchronous motor driving
the tape of the registerinE device. The functioninC of the
equipment and its applicability to the measurement of the
secondary electron emission was thoroughly iavestii:-.ated. I 1C
was found that the equinmr~ntaxld be used for sinEle-pulse
measurements as well as for ti _e investiC_-,ation by means of
periodically repeated pulses; in raxticular, it was possible
to obtain good reproducibility of ~he secondary emission
coefficient. The effect of the anti-dynatron grid on tLe
secondary emission current is illustrcted by the curves of
Figs. 5, 6, ? and 8. Fron, these, it is concluded tLat U 9
should be of the order of 100 V. The stabilit,7 of the primary
electron current is an important factor in the equipment,
especially when th-e de-celerating potential U is varied;
(~ard3/4 2)

1C '-5-4/23
The Problem of the blethod of invest_JF,"1_tijn of Secondary E7,-,;tron
Em~ssion of non-metallic Substances
it was found that the primary current as a function of U
did not vary more than 1 to 2%. Some measurements on the
distribution of the secondary electron energies were carried
out. The resulting curves are shown in Fig. 12. The Curve 1
of Fig.12 was taken for vi at U :3 = - VP (,.~-here Vp is the
accelerating potential of tl'-,e primary electrons); this (,u-rve
is in good agreement with the results obtained by R. Warnecke
(Ref.11), which are represented by Curve 2.
There are 12 figures and 12 references, of wI.JLch r--) are En~jish,
5 Russian and 1 German.
SUBMITTED: February 18, 1957
AVAILABLE: Library of C.Dn~ res~3
Card 4/4

AMMS: Shul 'man, 7 F: '- j -ovsi ,H Moro z Dv ,
'~u. A. , Fridri'--',,.ov, S. A.
TITLE: Secondary Electron Emission of Nic~cl (Vto-,ic'--,naja
elektronnaya emissiya nikelya)
PERIODICAL: Zhurnal Tekhnicheskoy Fi:~iki, Vol. 2u, '~r 1,
Pp- d7--)6 (USSR)
ABSTRACT: The task )f t1le present work -.var, to close the existin-i-
in literature re,-,ardin,~; the ener:,-y spectra of secondary
electrons emitted by metals, as well is to obtain data on the
distribution of secondary electrons acrordint; to enercies in
nickel. That is to say of all those which are erqit,ed within
the waole ranje of secondary electron energy at various V p
(enerT-y of primary electruns) of from 2oo to 2ooo V with
nickel. Starting- frof, t~ie d;~ta on the distribijtion of
secondary electrons accordin-1- to ener,-,ies the problem of the
importance of the quantities obtained at the investif,,ation
of t~.e basic dependence (Wiich churacteriz,-,s the secondary
emission characteristics of t:ie ziaterial - of t,.e depen 4 ence
of the coefficients of the electron e:-iission on V ) is dealt
Card 1/5 with. The -met'n.)d of spherical condense.- with a s~keric

Secondary Electron E_IiS8ion of Nickel
suppressor ~rrid va,,i used. The ethodl of t~~e
recordin.- of measurin- results, as described in reference
2, was z~lso use,,.. As result of the ii!vPI-t:.-,at;on the
f011017in,- c-in I)e .-,tate(l: 1) Tpvti;try electron. emitte! from
!h- rollector exerci~.,.e ~tn essentiul inl'iuence ori the
renults -,f :,econdary current in t1le ret rdin.:.,
field. The introduction of the su:)pres.-or Jrid offers t.e
possitility to essenti:tlly decrease t,.e influence of tertiary
electrons -Ljid thereby to obti,in, -nuch -:ore r,~liable data than
vials earlier tLe case. The (~istributi-_-n of t?.e secondary
electronf3 accordin,- to t~,.(- erier,,,ies of fro.-, 0 to Ve., a -,
inventit--tted. Co-,-)letc I:L,-, ciirve~-, for nickel -,,ere htained
rit V of' fro.-., 2oo to 2ooo V. 2,' In the sr)ectrum of the
.,3ec,)nd,,.ry electror;,,~ Jt is not possihle to draw -i ii--.itin6,
line between the reflected prirlary an~, the real secondar,
electrons. Apparently both kindfs of' el,~ctron,_; ure repreuented
in all piirtv, of tne spectrum. With small enerjies of
secondary electrons assumption thLt real secondar-.- electrons
are of do,iinatinl- importance is re!.--.soned. For the analysis
of the energy spectrum of electrons (of nickel) an assumed
Card 2/r border between slow and quick secondary electrons, equal to

Secondary Electron Emission -)f '-Tic:~el
1 17'70
loo eV, i~~ c~~osen. 21) The basic f-.ct rest.1tin.1- 1r.-,7. tree
measurements is that in V,.e spectrum of seconditrj electrons
of metals t~-'e relative number of lluicl- electrons c~n be
compared with that of slow electrons. The width of t.e
maximum correspondin.- to th~ slow real secondary electrons
is a little greater t;-!an wan earlier a.93umed. In order to
mart, the nu~~ber of q%tick second;-ry electr-ns ~-vi.-i-itiide ;Lre
introduced -,s follows: the p-;rt ~)f quio~ (,lectron.; in
secondary current and the rati) bet-,,ieen the :-.u:-iber jf quic'-
electrons und the niiallt'ty of the pri,:iary ci,.r--ent.
increases linearl,, uit- the ii-.,:rease of V., .Yid rc-cnes -a
to 26-;~o of tho tot-il n,7,br-r of 3ecnn,lary el'cctro!:.-. --,t 16,~O-
iZ-- on!., 1~ttl,~ tlc-enulent D-. V -Ind ia e,,,,ual t:~ --15,; 01, ti-'e
,ri-,ary current v-i'112 ~,,t 1600- 4~ The ret,-r'd%ti~-in v~rve:~ in
relative coordinates coincitle with one-nother if V is
~:reater than 12-;0 V. If V values are smaller the c--~rvesp
differ. 5) With all valueY applied for V -n refloxi:)n
of primar
7 electrons ta':eo place. The re?lectior. c-Dcffici2:-:t
at V > ~:'00 V is not realter t~,-n of totil ::1:.mbcr of
prizigry electrons. 6") Y'llien urinary current is in
Card 3/5 th- circ.-it of the t tr,,et i: t~ie c;-c cf r::)t C-~ i 1-t'~

L- - 1- I I/ .
Secw-l r~- Elcctron E::!ij,,.ir)n of Nic?el .1,
blaiikin-, of sccond,-ry electrorio for t;~e (-nef'i(:i,?nt o~
't (J" :. v % I'! - v, t - i!~
c 0 T" J .. ry e,iI
that ):* tot --I ret~r'-,-.tinn n" ::~- )n !lectron-11. 71 In
order to m;-,rr, -n ~f ~~Iovi clectronn t~,e
n e -) f - 1 ow
(coeffic;ent the emi-sion of -
electrons). As the existin: theories :);-l-- t. '-e i.,Ito ,-ccourt
the of second-.r el~~Ctron~-- bY electron--
..-n- ~,s inelastic reflecti.,n of .,ri:-.LLry el-ctro:~s :r,6 t`~e
foi ... i;-ti ~n of slow fecon(i.--.1-y electro:i.- with the -n.-Dtin of
2ccondary an', if inelastically reflectel ~:ri:.I~.ry
ele-trons arc :ot i.~to arc-,)tmt the Son
!,etwecn th-2oreticnl an' exi~eri:i-:;t-l c:Ln carriel
out th -,,if fi o ~ 2.:t ex:~c tness -re 12 f i -..,-e
r,:feren~c,!;, I-, o-' v.,.-Jc'. :-re
ASSOCTATIJ!" Ler.-In6rad Polytechnical Institute
(Le:i: :, ~.- .-)lite' n:.inhc~-, ~:,- i -ti tut
a 1 in:;-L
C a rd 4 / 5

-'0 32 C;/~; "
'let rov N.
'2 E *,ntalum and
yttrium Lx:.-,e- -n a tnerzoemisslon current
T E'X T 7o find t,.,~ '~.e
temDerature dependur~c.,,s o: e c t r on e m s ~i o n ( c o e ff I c i e n t
~,n pri:nary eleciron
C t n L a u tr, o r
L t. , 01'
ene-,-gy 1V the 'a rt,-e cn
F, 2, 2 , 13 4 2,
1 "L12 L was vL~i` ed r*ro::i j ev anz all
measure,ments veL-e ~.-.ace in
a r t: t swere
annealed at 120'~ 0 0 1 1
C ~ Y3 :t was;
found tnat , cies~411 c r~e i ~n r r e n T. so i t c,
10 4 + imes grLatcr tnar, I e1--,- vias temperature-
'lard 1/2

e,~ n I--!,- ry e i: f n
n (j,, n 1
s e c 3 n d L. ry
oi t
Concluded n c n
hi Cn - . . . - . L '- - I
t emp e r a tu r e
d istoi t ion -,C ~-,:-.nd:i ry
T h e a ri,)::j a ie,.;
Spec-4fic
1',,, t t r i Li:-.~ ox i do
ZI n'l
n e ~ e r. -; e n t
c- n c,-rrent nor a
., *. ~,;. n c e ~, :3 a r.*,, con,: i t -,-,n s for
!',,-,r j w i tn T.
u-, velated to
r e
6 S ~ C
Ka I in-na L n - .-r.L3'---ute e r
~c )be f, a r v
Card 212

4-
VA
AP30010 4 9/0109/61/048/00Q1045/1049 f
AUTHOR i.'-~Mdt6kovp Y4.--_A#
T11ME-.: Automit-ed method for investigating the secondary-emission properties of
materials,
SOURCE: Radiotekbnika i elektronika, v. 8, no. 6, L963, 1045-1049
A: TOPIC TAGS-. automatic recording, secondary emission, emission characteristics
ABSTRACT: Arn automatic pulse method for investigating garnnda=y~.Olactcaa
.~,-.,.-emission is discussed. The system developed for the purpose uses a pulsed
.,primary,electran beam.and a collector which is grounded through the input
resistance of,--a.secondary-emission amplifier. The beam target is kept positive I
in relation to th,e-&-r'ounded.collector whein the delay curves of the secondary
..~'electrons ate registered. Moreover, in order to eliminate the misleading effects
~-~of variations inthe primary-electron current, the energy of primary electrons
hitting:~the target is held constant by causing the potential of the electron-gun
anode to al.. Secondary-emission voltage pulses
-vaty along with the,t4rget.potenti
are amplified and -.recorded and may be viewed on an oscilloscope. By varying
Caid 1/2,

M287ZO -
AP3001004
NR.
primary-electron energy it is possible to determine the following charac-
_,:,-teris_t2,.cs. 1) the dependence of the primary current on V2) the dependence
-secondary current (these characte
on Yp of the ristics indcate the dependence
.on V of"the coefficient of secondary emission cy and 3) the dependence on V q
p
of t9e numb~er of electrons having,an energy greater than 50 ev (none last ic par-
-reflection fa tor) or close to V (elastic particle reflection factor)
ticle c
Moreover, ata given value of V
the gircuit makes it possible to vary with
time theAiffereace'(V,) betweeg collector and target potentials. This permits
investigation of: 1) he dependence on Vk of the secondary current in the V
k
interva. I - f roid +0. 11 Vk to - 1#I V , which yields the so-called complete curve of
and 23 the details of secondary-electron energy spectra
s0condary-electron delay,
as a function-of V1.0 '$In conclusion the author expresses his gratitude to A. R.
Shullmah for his help in the project." Orig. art. has: 4 figures and I table.
ASSOCIATION: Leningradskiy oolitekhnicheakLy institut im. H. I. Kalinina
(Leningrad.Polytechnic Institut,10
d,I SUBHITTED:-A4HAy62 Date ACQ: ]OlJul63 ENCL: 00
~CODE: ::SD OTMR. 001
-NO~RHF SOV: 002.

MOROZOV, Yu.D.; KORITSKIYP G.G.
Classification of instruments for electric arc anal electz-fc --'
I I _a:~7
welding and hard facing. Av-tom. svar. 17 no.3:62-64 Mr '64.
1. Donetskiy politek~m'Lcheskiy institut.

DRITOV, L.A.', inzh.; MOROZOV, Yu.F., inzh.
Thawing frozen grotmd with electric points. Transp. stroi. 11
no.1:22-24 Ja t61. (MLRA 14: 1)
(Frozen ground) (Electric heating)
0 1
I
a
a

-MQHMaY,-Yai.F- , inzh.; M24CHENKO, V.A, inzh.
Properties and use of cermet partf, in rnacninea-j manufapture-.
Mashinootroenie no.1 Ja-F 162. (MITIA 15:2)
1. Laboratoriya poroshkovoy metallurgii Nauchno-issledovatell-
skogo i proyektno-tokhnologicheskogo inBtituta mashinostroyenlyn.
(Machinery industry)
(Ceramic metals)

MOROZOV, Yu.F. [deceased]
Latency of the larvae of ?hysocephalus sexal--.uE 'M'o"n, 12,6~
k -- I
established experimentally. Uch. zap. GGPI 42:39-51 164.
(MIRA 18:4)

MCROZOV, Yu. F.
MOROZOV, Yu. F.: "The helminths of rodents and insectivora of the USSR
and an attempt at their ecological-geographical analysis."
Min Agriculture USSR. All-Union Inst of Helminthology
imeni. Academician K. I. Skryabin. Moscow, 1956.
(DISSERTATIcli i,oh rrih DEGR_i~t. OF CANDIDATE 1.1111
SCI -~ NCE)
So.: Knizhnaya letopis' No 15, 1956, Moscow

_y. Prrrisitic Wcrr~s. G-
USIT / Z(~orarcsitolog
'ibs Jour R-)f Zhur - ~'i , 1 55)5-;
.Auth~-,r __LjL,2_- U,_4tti- -F.
Inst -c+ givDn
Title Throe :;ow Hy en- i "i-IF 'r zubk- (S-r--() Tr~
r.-vy~, 'y -.t 1-ur 7,u' k-r!-kr,~shIrl.
Ori 7 Pul~- Urh. zrr. G-)rk--vsk. Ful. in-t, 1957, 19, 55_4~.
.%bstr-ct ~cscrifti= -n~ 'rnvin-s -f Hy
n. , C uc ur L 4 1 ~q i -~ s .- r e x sn. - n~l Di c r - nc t - cri - f'ur c!~ t -
~iLAricrl n. fr_,,~ bur-2uuk~ -' tho Yfk-.11t S F
Cr r 1 l/ I

MOROZOV, Yu.F.
Discovery of larvae of ?4acrocanthorhynchus himidinaceus
(Pallas) In dorbontles in the Byalovezhaka Pushcha. Dokl.AN
BSSR 3 nn.10:430-411 0 '59. (MIRA 1):2)
1. Prodstavlono akadernikom AN BSSR V.A.Loonovym.
(Byalovezhska Pushcha-itcanthocephais.)
(Parasites--Dung beetles)

MOROZOV, Yu.p.
Two now species of nematodes from rodents. Trudy Gel'm. lab.
9:196-202 '59. (MIW. 13:3)
(Megino-Kangalasskiy District--Nomatoda)
(Byalovezhaka Punheha--Nematoda) (Parasites--Field nice)

MOROZOV F.N.; MOROZOV, Yu.F.
$ s
%rphology of the larvae of Dictyocaulus viviparuB (Bloch, 1782),
D.Eckerti Skrjabin, 1931. Uch.zap.GGPI no.27:13-15 166.
NDA 150)
(Nematoda)

MOROZOVY YU.P.
Bio]:O-gical cycle of PdctuJ-aria amurensis Schulz, 1927
Rictu-lariidae). Uch.zap.GGPI no.27:1?.-28 160. (~'E. -C.-,
. ~' -L ~'. ~';
(Nematoda)

MOROZOV, Yu.F.
Changes in the 87stem of the family Phyealopteridae Lelper, 190~
in connection with the study of Pseudophyealoptera soricini~ 6a-' 119,
1914. Zool.zhur. 39 no.3:327-329 '60. (MIR.A. 1~-6)
1. Helminthological Laboratory of t he U.S.S.R. Academy of Sciences,
Moscow, and Wild Life Preserve "Belovezhakava Pushcha", Brest region.
(Ifematoda)

-140MZOVP Yu.F. [Maxozau, IU.F.J
Helninth fauna of bats in the 3-mIcvezhska Pushc~A. V-s-_sf AN ...
Ser. biial. nav. no.2:92-98 161, __: 7)
(BYALOVEZIISKA FUSHCHA-WO"IM, INTESTEUL AND i-LASIMC)
(PAi-ASI TIZ -BATS)

STRYUK 3 ~-.O-~ -o VA , A 1". red .: 3~~-, I VIA
K V re-J.
[Ex~;io~l tion ,n ".,.a opref.,~ W, I r,~ -,rlkfs
m~- r,,9 a ruWebo--,)kl Tematicheskaia
in
v:;z3tavka "Skorcstlnoe prD-;edmie j.(Agotcvitq!lrr7Kh '.'Yrh-.
botok na ugcllnvkh shaktitakh SSSR".: ~,.utew)Jllte-' r
skva- 10,b'.. 88 p
SSSR. -al *- ny), nau- ss sk 1, y im~* 1
i nf orTna ~s i v urc
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30381
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q or 2/:)'1 or,
r- o Z'., v , Y u . I ir-, A P e '.- r-, A A E
).A
L-'-' A rnpiler-type pr~);,rauiratr,~- ;i- ~;em RCK-- P.,
P-)("Ieuly k 1 -, e r r. e t JL k -1 1.",, )w
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4 r e' ~,L 'uy ti e iuthors. L, F, Kovaleva, V K f
h e - ~3 TIe syste.
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r e t e n T,. e b , s i c -~ :)m p o n e n
t ~3 t-i r - e ~A 1) 1 r i) 6 r: i m , i n -A
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s ~ Th e s ys t e:-~ u s e s t h p e r,-, mc. ,:):1 (3 f
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.e Tiie of an opera-- t,)r r.errle, ~~i'cwlr--
-j I d t'~. e links bet,.t,,een them, is 11 f i e fi i-; t e i P. r;
f:1-1 t l _;,,-i -,Y-l this jc".eme i!i "Ljaded 1 n t -) ~Ie omp er- j
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v e ~ ne 1 orre s ond ing s t~inda rJ p co --r-ims in i~e 1.1 r:: ry

30381
1/1'000/00: / 0 0
milller- ;Je D 0
;perators) w) I 1e others will h;ive t,,) be focmu~-I!e,i -.r~ ~l
s t~i nda rl -D pe ra tc rs Th e I i b r~i ry .--o rit:i i
Lr. :e ma g i I ", i-..e r% t io r. s f r ex e
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exe-- tes fill
'he f i n a r- m n e
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er
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r. Do i n eq. _i a -
an
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S//1 94/6 1100011012,1101 ~-,/O-,7
D201//D3071
A'jTHOR: Morozov, Yu. I.
TITLE: Standard programs
PERIODICAL: Referativnyy zh-.,~rnal, Avtomatika i radioe1ek-,,r,.)nika,
no. 12, 19161, 4, abstract 12B21 (V sb. PrDbl. kiber-
netiki, 5, M., Fizmatgiz. 1961, 117-15-,)
TEXT: Some ideas about standard programs (P) and about p.-Dgra=-
ing automation are given. For the problem to :je solved or.
tal computer it is necessary to set up the program from the alg.9-
rithm of silution. The problem of program automation consl_.';~S in
t~iat, hav-jing assumed the necessary information ~ibout the gorithm
of the problem solution, the P be obtained by means of -~:-e -.lac~line
itseif. It is shown that the efficiency of the method of programm-
ing automation is determined by the simplicity with which the ,n-
,formation -ibout the solution ;11gorithm is as.9LUTie(I :i:A' by the ea.3e
wit:. vi~'.ich the control of assuming tile information to it~(_- true is
nieved. Application of standard P represent,3 gre;i'L po!.;~~ibillitie'-~
Card 1/3

in satisfying t,.e tw-, requirements :ib,)ve. In e i i
durd P's are subdivided into groups accirdin-7
features: 1) For what purpose are t?1e s-,an~ard P
,.Ii d of' (~.,ie in their Lpplication. The diz3c-ussed
It (I . I ~ ;'qiiown
ac c -) rd i rij- to Wic f o I I ow II I ) .211 bt, I d I it ry ,] Litrid; rPt
that setting of any subsidiary P for the given )?113 1~1 :ti.
!iry oijeration. It is recommended setting up P, f,,,z, t:e
essary infirmation is supplied always in t,e same ~t:lj
form; 2) standard P for increasing the computer -,in-7e of -j
0 p e i
tions. The set of elementary operatio-.s a-d ho,,.- ob%~,a,-n
these more complex operations is given; classificatl~)n :f
.'bution of information in memory i3ystems. Trie ~,on--e~-t -f -n ~pe-
r,it,)r !t-,d of )per-fitor systems is f~iven. 'Phe e
,-,on6idered: Symbols and notation, the description -~f
certain commands of the "Strela" computer, stard--~rl
units, classification of information,
system, t"le concept of P operators ~~.nd oper7tt3r
d-urd P numerical solutions of simple mat.-,-emu~i--a-' -r-- e:::
bard 2/3

S/194/61 1/000/0 1 -,'0 -7
Standard programs D201 /'1)-7 ()7
.1 1~
standardization of program acceptance; 6) processLng of st,-ind%rd
P. The following problems are considered: Externally ?recessed
standard P; self-processing standard P, amalgamation of 6rG:.~p
of standard P into a single standard P; 7) automatic pr,),-.-a::ImIn,-
of arithemtical operators; 8) automatic conversion of st-ind:ird P
into a single P. The following problems are considered: StAges in
setting-up; the standard P library, pseUdo-command, p.3e-_,do- - ode,
pseudo-program; compiling and interpreting P; 9) program -outoma-
tion. Programmin,- systems. / Abstractor's note: Complete 'r,ins-
lation.-7
Card 3/3

0 0 0 0 6 k7;
4 4
I' k j V Yu.
-;e! t
L11 m -Lj 1 V
In
t 11,
v , :
t
rl t '0
Du h,
1 c to be t up in t~5 ts n rcj
t l-, al I ti Ull PLJ in t frum tn(! wh I I
cl
t- t U p LO i' t~ r th, choict of the .,.not cne puts up the
112

A do- 'U:' o t
L' t u c Lo t Lii
b,: t i Lu t t n - L V;
~,Y. iLL5 ~i
if, 'd0t,il L 1-1~ cc a
i c n Ti S P;l - T~ie b 1 o c k - d r LLm c r:.
Card 212

7 1
10 57/6 1 /C
9, 3 -D 3 2 -~, 7
AUT-O~S lmjhenni~, 'I.
TITLE: Analyqis of the i'y nr e5
in an elec'.T-,-)n
PERTODI'AL: Z?Uirnft' n
TEXT In cont4.nuat-"-,:, m P. cross (p'-y~;. '~QV. 7~.
1851 1949), A. 1. Akl,4 1, 7, 7- 7 ,1 1 and
C. 11. Gordevev (Zh
ty c s --a n
01 longitudinal eieo'ron 'he t-e
velocity of 'he z i 7n o-t"'
ve 1 o c 4 to f o 1 a s ma el ec '. rr~:
J,T. Ye. 'Iertsenshteyn, --e -n- re n ro -i I s
4~ 7 1 e,I -.I
where p iQ) ; t~e lis -,n r-; 4s
Card 1 1/ 10

Ana ly 9 1 s of t he ah, i
f 0 n 0 ex T), exp
V
0
cc m n 'M n e n o t eo the r t c' e~3, m 'he e'ec*r,)n mags,
1/ 0 1
n1 the density of the b t-- !e!~fiity of the elec',-,,~n olasma.
and U the beam veloci-~.'~
is obtained from -!nd "2), -r--rp
L/,) I /I T V I k,, T, k U
'u u 1"
t I
~2.
7
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en') e s r: c
inves,.jgated
integrala
app! ied to t,-e c:.:-,
fojlOW4
from which
0110",s for
at
7/jn

An a I y s 4-9 o f t-i-
follows. -~,here
excitations. Fur"".er:
2
(Fig. la), where
o
Card I,,/' V)

Anal vsis of the ns+a'b-'
3 2
3 3~
2
-3
2
For a =1 one has
1718
- 7
)n(? n s
Assuming and using,
1 -4-
-4
xM.. -4-
0. 1fl, V.
3
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23718
Analysis of the ins 'abi. t-,, ~~f 37--3/3207
In accordance with (7),
If, hovever,
S_~ e -:U4()n3 lee,, to
l ~9)
1/2
'Ka)
2 2
k
is obtained from (3) in first Tnis permi-*6s a simple
estimation of the maximum y; is -!-tprmined 'rom the condition
2 2
-1 - -: I on
so that for , , find.9 7' R. I. Izraileva
(unpublished paper) deter--~ne'] -~.e of the range of vibration
s-,D7,s *~ie de-jendence of t-e 14mits
excitations on the basis o-- 74g
Card 6/10

7 Jd-
7/6 1 /r, 7
Analysis of the instab` I 1 3 27
/TIN 3
on at a
lower uDper ro ma.
The comparatively pgre;zt d f c, :7 e n r d 4
.11 VA '0 kin e r
(18). if
n a exp 7 t 1 n,~i Px~) i k."r + nt,
0 0 . 1 1 ; k-,
is substi~utel 'or D'* t--.e asm,! and c
-4-4T
~.2 2 (21,
C 0.1; 'Z it: n
f -n
f ollow e ~ rom- the hyl r,) )r, ~: on ~',;e ~ism.~n-)tion t--~'
lor the --,mnlitude -;nl inns e' e c t r-D r, 1- e;!m, e a m
If only a 1 (el Pctr,)n e,;,i:i t 4~ on
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.3718
Analysis of tne inctpl,) -~f q
E E, ex p if ros
lobo .,31ex 1) Q.IIIt C OS
-0
po noE, 3 e x 1) COS T.
2
12 3 2 7
(22)
(,()s _4 T_
U = Eo exp 2
2
uo = Eo exp C03
0 2 -T
is obtained for the P-11 Pc --ic f~ --i for velocity perturbations in the
plasma u and in the beim Ii, i:~ the cular case of an asy-ptotic wave;
0
here
C. T T
3 2
,nherefrom all other proDerties of t-e %,,eves can be deduced. The authors
thank Yu. I. Xuznetsov, L. I. S~iibarsh--;v, Yu. A. Romanov, E. Z. llaar,-lmov,
V. A. TeDlyakov, and G. for va:uable advice. There are 3
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"1 37 18
57 2/C I
Analysis of the iistability of 2 10 2 0 7
f i gn-ires t,-tb le , and 6 re S-v e I r~d n n - S
S 77 ~~ 17 TE, D September 161,
Legend to Fil~. la:
--ax' /ont'
G X~-
13
65
F1
0' (X
92 04 95 19
06
0.
06
32 04 C6.
Car,! 9/10

71, 3
lof radiational,hydrodynamics-for the general relatfvistic case was written by
V. A.- Prokof,yev (Uravneniye perehosa v relyativistskoy radiatsionnoy Sidrodinamike'
DAN SSSR, 1961i 140, str. 1033.). In equations describing motion in a medium
radiation- occurs. in.the, form of a divergencetensor of energy-Impulse radiafton.
Generally-speaking, the form of this tensor is very complicated and must be con-
sidere&simultaneously-with equations of the medium and the equation of transfer
of radiation. Under conditions close to equilibrium, this tensor can be computed
!by successive approximations. The authors consider a general.equation obtained
from a stim of tensors--mediun.and. radiation., Such a procedure greatty'simplifie
probIgms of radiational hydrddynamics.I.By restricting-computation of the tensor
to the seco#d approximation (considering hydrodynamic variable
l. terms
linear in the gradient) a generalftation of the approximation of the radia-
tional heat conductivitylis oLtained by introducing the mean according to Rosse-
land; see S. Chandrasekar (Vvedeniye v ucheniye o, stroyenti zvezd. M., IL, 1950)
'and D. A. Frank-Kamenetakiy (Fizicheakiye protsessy* vnutri zvezd. M., Goa. Izd.
f I%. ~ma t. lit. J959). The authors 6om ute the tensor of energy-impiulse of radia-
p
..tion in this.approximation. This tensor was computed earlier by Thomas (op. 0
ibut"his computational procedure is nonstandard and-leads to a cumbersome inte6t,.A.
Card 2/3,
T

ACCFZSIO14 NR: AP4034267 5/0207/64/000/002/OW8/OGU
AUTHORS: Imshennik, V. 3. (Mascow ); Morozov, Yu. 1. (Moscow)
:TITLE: Shock-wave structure including momentum transfer and radiation enerd
i.)MURCEs Zhurnal prikladnoy mekhaniki i tekhnicheskoy fiziki, no. 2, 196h, 8-21
TOPIC TAGSt shock wave front, radiation transfer, absorption coefficient,
radiation hydrodynamics, shock wave, viscous discontinuity, radia-
1
ition equilibrium, Eddington method, diffusion approximation
ABSTRACTi The nonlinear problem of shock-wave front structure with radiation
transfer at relatively small speeds, when 0 - v/c