SCIENTIFIC ABSTRACT FR:MALYSHEV, V.A. TO:MALYSHEV, S.B.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001032000044-6
• Release Decision: RIF
• Original Classification: U
• Document Creation Date: November 2, 2016
• Sequence Number: 44
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTR

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~`a~ca=q;z~~tcy,'::-~chuaa*ta~t;~t~~r~.s~;a.cs. ~`c~. (;5} was cl~~dciceci roar th~E ~r~aa of
'~k~:ta! ~~t:ot�c~~du~~~~.~r~,,~y pat"' Gf~~', us~i~g aa~ sarnplca!s indttas~tx~~i.u]. Pt~ato-
t f t ~ ~+~;$~z~~ar~~ t ~ ~_ -p;~, ~~~~:} a>r~d ~ ~ ~~ (~`S*~K~~ . ~~x a~r~rnan~~i
~~ ~ _ ~y ~
, a ~~~a~r~~f_ th~~ ~h~~ ;~ilYUta~�ch~.r~~cta~r~.~t~~.c~ o�" the~+~ g~hat~re-sa~~.s~tc~r~ w+~re
~ r ,~ ~
{~ ~ rF.' sub~tt>>~t~~~;~r `~l~a~eAar w~ithaz tl`ia ~aho~:e at~an~~ of values ~-f hale fight
f ` ~~~~ ~ -;wh,~n ~~~,s~~:t~cl As -~, = ~ C`~} . ~'11e ~.~:gt~t 7,seir~iat~ from ~
F.,
` ~~ i~r~a'Gteat~~~tc.: w~Gth experimenta:~ data gave clo,sc~ agar~~elment when
" ~a%r~y-., was' ~lotl.e~d' a,~ainst ' F~x1 , At low �requ.encies #ha
ex~~~ment~Z p~>ar>f`~.~~41.I'#'S. ,
,: _
t; _
I1~5C},~rAT~4~' ~ - Te~,gc~rtro~s'kiy rr~,dica!teltihnic;hes~Cy 3,at~stitut
~. ~ ~(~Yaga;~nnrag ~iadi.otc~chnzcal Snas~titute~
�~ ~ S~J~~~x~C'I'Ei~~s. �'; Jan>`tary 3, 19b2
,_ ,
'~ ; ~~'rd X13 _ ~ ~ ,.
t ~~ r ~'
~r~ ; ~ ,.
~ ..1_,~.,_W ._ ~.:. ~.,_._.:...~..,~,._..._:._ ..~._ __.: ~ _._
..
~, ~> ,.. -
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--
~~~ ,, ,. _
,..
it ~ _- ~ _ , _ _"
,,
~~~S+er~m~gt~t~~:~ ~~icct~~.ir~g.: u . ~ ~202~~4~(3
fre~quericy f ; c~r~d' ze~a ~'reque~~y r~espectxve~,~y; ~ - l~ifetin~e of an
axe~~troh i~X an ~~,~;at~d Mate, f -', ~'x~oquency. df the squaro wave ,
pt~~..~e~ .;�~r~c.cIi~~r~,~ the luma.naghor, P~. - .rate o~ generat~.on of the "
,cturrent,. caa�,rie~s der un~,t vo~;time due to the ~,rradiati,on,
~c~'�-::~rrcaba.tr~~'1~,~~-_:Q~;,_~re:cc~~ibi,n'r~t'aL_on a~ the o~trr.en~ carr~,er ~.h a unit ~ "
;v~rlt~a~e ~,~.t~~:: a~i~- "~a~ the- r~ecc~lnl~inat~e�' c�~r~ter~r; a aid uo ,~
`~~i~E~~~~ur~a~;:o`~� tlhe ~k~otoaanduct~~e pu~lee~, cd ~orre~poindi~g to
~t~~e~ `2~ir~a,' ~'r, c~qu~ncy of irradiation. ~q. (4) was checked. for the
cae~ of ca11'tode,, 7.u~ri~tnescence of Zn2Si�1~�Nln w;nich ha,s e;cpanentiaz~.y'
deot~y~~tg, ~tam~.nascer-~e r Cathade ~.tiunix~escence was studiod in a
,.
f~~'_5'~ .l ~~'~'e;a~ tube which wa8 r~c4r;~orated iii; a e~.xcuit contain~.ng
t~ er~,ut~r+~ ~r~-ve pt~~.~;~~ ~genQra~or and ~ ph~t+ae~.`ement ~~k~ ~STsV) ~`~.th `
az~ p~c~1la~~co~ig_ ' -Values of z ,ineasursd at a fr.equenc~r of 1D c~
w�r~ ~~ ~~.~.:;~ t?.'Ql~~ ~i,p-2 sec� ~t r~a$ shown that with the
~~o~`f~.c.~er~~ a~ f`i.;l~,~.inig: 1j ~~5, ~h~ d~G~~~e~e of frequency did Hart
~,.a~icr,ea~e .~Yre 'nm~-iittidQ of the luminescence, .hence knowing T and
too ~~,`~a~~...~a~~~i~l$ `~o date~m;ne , I. y ar;d /~~ far each measured
^~~iue .off f~~egt~~~.c;y~ , .. A ~ra~hical ~^a~~par~,~a~n. showed Sock, agx~eemerit
bet~-yee~, thFS�"+e~pieratu~enta~: and theoretical reau~,te of ~umine~scence
~arr~ ~;1 ~3 ,
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;~ta:E'~rs
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~h~~~cc'~tari~tcs ~a~"~~'tttrfiar.a~ista~rrs tend lumi~~~~phors
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ara' tht~'
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fi,~f~v~e~ - ~~~. ~~~ .~ ~... _ ~
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x ~ aa~~~ed axe use a~' t~ua ~;E~eo~t ~ ~~ ~~l~~rat~d w-~~ ap~~f`9,a
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r+
Symttetrical stationary p;roblem... ~10~f~B1B6
if the boundary conditions are v~~r ~ v1 and if v ~ rmr ~ v2, ~~he gas
1 ~'
~:
flow through a cylindrical surface of unit length is obtained from
v~
~ ~ -D 2n~ d (Inv) __.. 2nD In vt
~� ;
The solution of (~) for ~~ stationary central.-;~ymmetri.cal diffusion takes t)~e
form '
~_
J ___.._...,..~
subject also to
-9nR Du dR RZ - K1 In va
(11~
if the bol,ndary conditions arc analogous as above.
ASSOCIATION: Taganrog7k:iy radiatekhnicheskiy institut (Taganrog Radio
Engineering Institute)
SUBi~SITTED: March 20, 1962 (initially
Card 3/3 June 26, 1962 (aftex revision)
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r
~ v
nUTiiOR ; S 5 7,/O2;,'p ? 2 ~,..~
alyshE.v, ;,r, ~~ =+~~1SG
TITLE : -
Symmetrical stationary ~rob1E,
PGF~IODSCAL: Zhurnal 1 m of isomer
tekhnjche3ko mic t=,~ts ci~:i'fusian
TENT: 3' i'i ziki ~ v.
The stationary solutio 32, no' 12' ~9ti2, 1
4~z,~~8~
n of the total di `~ferential ~: u,
Q anon
~u~2 (In v) :~ ~: ,~~ s
~~~~
3n~~2~ Cl ~ m ~ ..,.~
desorib~,ng the isothermi~; (~~
diffusion of a single-com on
P ent
"`-- ~,as is ;studied.
'~ D~3va~ v~ ~ kT,
holds for the ~ ~2 na2v(1 ~ C (3)
diffusion caefficie,nt~ ;vhere 'n
' Card ~~~ T -
is the mass of they ~mo:l~:c;~le
~ ~
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s/~57/~2/o3~/c~o3/a14/o15
Ufiect of scrption on kinetics... ~139/yiO2
~ dn~ di~~ ~ v n - ap. lience the gas afflux to the system l;~er second
~dt:t u dt; ~
~;�
he s~~atem. .ne ~~ressure
'-~ = k1q(,l n - ap} where q is the umption of a umiform
smooth cathode, two criteria arise to te~~t this assumption,
The experimental anct thcox�eticaJ_ val~~es of C cnust coinc~.de;
the slope of the current-voltagc7 chc~ractcr.i~;~i..i.c must f. ts? :law t}-c;
"three halves poi~rea^ 1.aw". :fit i.s claimed th,.~t non ful;C.illnc:nt of
these criteria gives a measure of the non-uniformity a:f the
cathode. The autl.ior points out that errors arise due to finite
dimensions of the diode and that; these errors will increase,
Card 2/3
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s/141/6 :/Ga5/o~~l/0l3/0~4
~za~iE4>7
~~ ~~
AUTHQR : 1!,a l y~lh ~=v +___~ '~'"'
TITLE : Theory of plate diode with a uniform ca ~ho~:l~e un~ er
satur'a'tion conditions
PERIODICAL: Tzvest:iya v}~ssliilcl~ L1c11ehnylCh zaveden~.y. 1Zadiafi.zilta.
v.5, no.1, 1962, 1.21J'-135
and
TEXT: Tl~.is paper was Presented at the Conference of PIV
SSG SSSR an Radioelectronics, IChar']cov, 1961 and at the
7th Scientific-Technical Conference of the Taganrog Radioenc;ineering
Institute,
f1 cluantitf Asuccessz�c aT,ra~;ia~z~;tiu2z:3. ;rl. (~1 ::o� rc�~cul~s
in a systen2 of 1c+1 eaa~,;;.o~z, of ti~.c ~yj,o;
y ~� Fy (U�W~ U,,U,,...,U~') e -1l ~ cvo .w. u~ u.,.,.., ~~h >~ + -~
Y
Y
i~.xere l; is. the nuzn'ac~r of izarrzona.cs ~vliicll r,escrzLe the
process, I~, is the c~sciZ~.4i;uio21 cY2~iz,ac~te;risLxc of tl2e non
1.a.near elc :r:zt :~rit12 respect to ~t:he ~~~th Iiarc;ion:ic and b.~
la. the pl2a.~~1 of the rteu~~;ive ac:::iit~Ga2zcc for tili5 i2clrt.tOlli.c.
These tj,tl121tz':.xos are `riven lay:
Card 7~~.

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X4378
' ~ Method of . , .. ~~'~.42/60/04~/Q0d5/~JQS/C~,S
~I.~2/Ej~,2 .
the amplitude and frequency o:f the ~ex2erated oscillations.
On the busi.s of the A.I. LyApunov thrary (Rey,.
' ~' S - ~vosdovQr,S.ll,
Theory of Electron Devices for Ultrahigh Frequencies, G.TTTL, 1956)
the condwtion of the sta'oilit~* of the oscillations is :ln the
form:
aUCF~U�U ~~ c~s8(Clp~~o~U)~ ~ 0.
... ~ tlo).
if this co7~dition is diet for any U smaller than t~hose~ '
deterlLiixxed by Eqs. (~~) and (,,) , the oscillator operates under
conditions o:f "tl~eak" excitation,
self-excitF~tion condition roc1uires~tl~~,t~ �tller 12and, the
c .~ C
sah er a
Card 6/13

(ll)
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i~iethod of ... ,
where
2~-t.~~~
S/ let 2/gyp/C}C3/CG5/Ot7j/U~, j
f'Jl j,'/ L~ ~~ G
r �
F(Uo,w,(~) e' i la tu~~w,u) + x1 ~~',~f ~- iwr qr
a (7a) .
1:n tho abc>vg c~acp;r�ssion tf~� inl.tial volta,o ~~hASO zs a.,ssurned
to Ue Zerc- and Uo represents tl~e operating po1.n~. The F
function r c U
~~.
. ~'
�r'
;~
~-,,
an a referred to as tfce oscillation eharncteristic ~'.t,
ow the oscillator ai~c? tf~e quantities r U
the modulus and please of t~2e '~c~r ~ and b �repres~ant C''
~at,.ve ac,r:-ittance. I~`~^om ~q� (7) ;
it is found that
J
B f / ~~) ~~-
G ~~ t~ la (UO,w,~/~~~ ~~
(9) ~/.
rl
where G + ~B = Y Thus E ~ f'
q-~ � ~ ~) ~~nd (9) fully d et err :in e ~'
Card 5/1.3
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24378
S/142/60/003/005/005/0l5
1`1st:iod of .... E1;2/ E382
where 1~~ is the ~ -tI1 co~aap~,Q;, 7iaa:~u~onic of thca funetioal ~i'~ .
If ,it is suf:~'icient to consider lc Harmonics the equ~ztxon
can Ue ~:rritten as:
' r7~ k
y~ ~ U T ~~ ~- ~wvl (p r_~, ~ ~pe~,.nr 1 ~'~ ,~, 0. (~)
y' ~ ICS! n-_A 1
The above equation has 2,: + ~ unlcn~,~rris vrhich ~.ncludQ tk�,
biasing volta~~~ component Uo , amplitudes and pha,~es of th~-.
harmonics and the frequency w of the fundamental. Un the
basis of ~T;`ct,~ aUove eriuatioil ii; is possible to solve the tt~ro
osc~.llator problems. The case of a single-harnonic &ppr'axi-
mation is considered as an example. Tn this case, Eq. (G) cai~
'a e r epr es ent: ed as
Y-}-F(U~U~(~e-ltacu.,m,u~+At ~0
Card 4/13
(7)
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� ~
' 2t~378
� method of .... ~/~~~/~0/003/005/oo5/ors
Ez92% E3$2
� The method can be roferrnd to a~ thv !n�thod of spectral ,~ ,
lxnc:ar~.antion: An aac3ll.atar can bo rapra~onted in tho form t'~
of tt~o bipoles: a nonlinear bilaole cor~tainiilg the nonlinear r-�
element H ~ (Fa.E. la) and a linoar cl.emeiat reprosentin~ the
oscillator circuit. Sacneta.uzes , un o.~cillator circuit :Ls
ropresented in the man~,ar shoi~rrt in 1';i~. lG� but tiais is
.~
~.
equ~.valent to tlz� circuit xn Fib;. la. In tlxA follo~lr~.n :tt ~.a ,
a~asuniad tl~at the oscillator circuit :i.s in tale form s~hoz,m in ,a
' Fib. lE. The nonlinear Qle~;xant is a;~uroximatod by a fu7tct~.on ~
i :. ~ (U) , where U ~.s the volta;fl. Tne K3..rchlioff ocluat~,on ~~
for the ay~tecn is: _~
~,-,
d'U 1 dU 1 d+b (U) 1 ~
dt' ~~ dt ~'~ dt '~"~`U o' (1) 1 ~
r
� ~n $aneraY,,, U as a functio~l of tia2o Gan ba raprncented AB t11e ';~.
Fours or s ez~~, es : -~ n
~~ ~
Card 2/lj ~'
~, r}-
^y, J
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-...a,.+.....,..-,.....-.....-+..srr.~+gM..'.-..~~dii may...... .,
...~,~�..~...-aa..,,,d~'''57~.,...,au �Iwo,,,-~-........�. ,~..~.-s=b.". ,., _.PC,,,,..-~,,,,,,.~-�---.._. _ .._._. .�. .
9.3~Ld
AU'fH0 : t4Alyshev, 'V. A.
T=TLIJ: ~~lethod of Spectral
of Oscillators ~rul
P>{R20D1CAL: TzvQStiya
l~di t 11 '
$/ a.42/ 60/00~~~~,/005/o~.s
~1~2/:~;~52
L~.nos,ri,~ration in the Ti~c~ory
SomQ of :Cts Applic~xtions
vysshil~h ttciZObnyl:ix z~ivodQn~,y,
o e~in~lta, 160, V'ol. ~, Via. 5, ~p� ~71k - 1f~5
TEXT: The general problem in -L�ho t:ieory of oc~c3,l~.ators,
t~ith ono nonlines.r element, consi:~ts of solving the diraat
+~nd indirect desi,n problor,~e. ~`Iia f:~rst proble;us con 3~0
formulated as foll.o~~s. T+'or a ~~.ve~i .~ozYlinaar clement and
~oscill�~tor ,system, it i;~ noeQSSar;- to determine the sh~~po of
the genera~tcd oscillation~r unc~I +:I~o f:~ ocltioncy of tlaa funcia~
tnontal harcnoni~.- . Tii� second pro~,lezn r~l,uaunt~a to the
doterminat.Lon of the parametea~s of the nonlinear el eraent or
of the oscL].iator circuit which z~raulu produca the desired
rt+raveform acid frequency of the oscillations. Tn the folloz,ring
an attempt is made to tacl~le thew P.~�o'nleais by employing the
mothod dov~3loped by G. Ye. Z'ulthov (Tte;l,. l: Comlalex Variable
Calculus and alts Applicat~,on, Taganrog, 1g56) .
Cmrd 1/7,3

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...
,~' ~~ f
Experimental Verificati ,
/. ,%J.~f~~ '
i
on E~f t:}7e 'r
Os~cill.ators with R� 11r
,~
of UlCrr~(-ll
~h.~frc,
,,
5ena1>,r.e Lr~:,~'in~~ t
~~
~:,~r.4,
~:alcula�~ac3 ~, ~ _
�.
~j}lC
~
{
~~)(~1
}.fUf'lllit.~.
thE~aretic
l ~iS):i.Tli:`~s ~~i4~,('~~lf'T' W.1.t~1 ~;}-t~>
a
line, for the function
illu,trated in Figs
2a The given b L
y ~~ d4}, aa-e
::urues of fun~tians exprF:s;,eC}
by Ec~s, (3) and (4) are shown In F
�
.
the experimental points, while +
h i~
, :3 , thc~ ~::irc.~ e-
~ denote
s
e
-al~ulated ~~urves~ The "solicl" solid lines show the
c.t.t.r
the i~un~crion of
~ ve of Fi
'~~ ~~ repre,en*.,L1~
L
of Eqo (() the ,yxr1~'e;,, of
i Was
~
~#
g ~
ca.Lctilatc~d on t}ie E~asx;;;
.
,>
From the figures :it ~.:s Lon.cluded th
~i?%e giue the experimental. points,
at ~t
3
~1

carre~;t resu~,is~ The a.utlior e
~'
N ~
�
)
and (~)
x
re
(
~
~ FaktoroviLh and G~A~Io avinarev p
sses his ,~rati
tu
de to
f
out the _
experlment5� 'I .here are ~4 f
z~efere or their rie..p Zn carrying
i~;~llres ac
d :~

n~es~ i
soviet
ASSOOIATION;; TaganrUgsiciy rad~_otekhn.t she
(~~~ '~.~~~r Sk1.V 1T1t1}l.iF
,~i (, ~ i1((1 U ~ 11!1; .! t l N t~ 1" ]_ tl E?' .~ n A3 * i ~; U �. C}
SUBMITTED ~ November 5 ~ 9~'=3
Card 4/4

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�.
:f~,, ,
_ .. ~ ~ ~ f t 3 t) ,j ~~ l~'.~ . ~ ~ kJ .~ i3 ~ 4,~ .~'..l ~" lz_,'..
Sim ~ a:~UC7
Experimental Ver:ifi::ataun r,t i-,r, 'l ttc i>ry c>f llLtrahi.~ct~~it~~~ltr'rtr;,
Qz~c.ill.ators with F{eaorir-rtc c~ I,c~:~ri rt,
reson~-tor~ In the earlier svor�lc (lt~t_ � 1) ; i i. w~~:-t ~.;1.;~r, ~~~iir~~vjt
that when the z:ouplirig parameter f ~ 1 a ~l~ sc.on#.:tnu:l ty .~ ~
in the wavelength is observed; this is detertn~ned by Eqs~ (6-.,
The v4tlida.ty of the grove furmtaatle c,ti~s ~:hc~r_l..ed expc~r.irnE.ntr~ll.y�
The experiments were ~cirraec~ out, on a lcl.ystr~~rt where: -klte~
auxililry resona#:or Was ':C>IltiE'.~, t�?Cl t:c~ Lf1c~ prirlc ipa7. resonator
separate~.y from the usexul. load, Ffrsr, tfic~ c~uantlt~.es Qoly
QB1 � QUH2 ~ Ql}2 and ~.~~ �wer}~ de tc~r~trriit ~d .f cry, a co Ld k:lys Iron .,
The attxiliarv resonator was then connewtE:d ~o the p.rlnc~pal
resonator by means of a coax.>.al 1.~.ne and the Leneration znne5
were obser~red an the os;:.illoc;raph� 13y varyiri�~ Al ~~t~d ~~
it was possible to obtain symrnetra.~ca1 zones and to study their `~
characteristi~-s~ The experimental rescxlt,s are shocvn in /
Figs iW4~ The function hl :-. f(~3~ } i.s il._lt~stvratc~d rn.
F~.go 1 (see Eqa 1) ~ The ~.ircles on the f::ic;iire i.llust.rr~tc~ t~ta
experimental points; wl-iilc tl7c ytr~.i.trl~tt .l.r.nc~s show tlic~
~:,~~ rd 3/4
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li L~/~J ~;/11

85999
~; '~
AUTHORS Malyshev~ V~A~
TITLE ~ Experimental Vera.F'i Una t.iurr .,; s~'~ic 7'h~~ox~, ;. ~ ~ ,~a~ ~ai~ .
frequency Oscillators with ltesoriarice Loadlrr.t,
PERIODICALS Izyestiya jryssh:ikh uchebnykh zavedeniyy
Radi.o~fizzlca., 1960� Vol� 3, IVo, 3i pp, 452 '~55
fiEXTa Tlae oscillators oonsidered a.rc: t,har~cter.i.sed b~y the
presen~.e of an additional reslonator which is ~~oupled to t~'ic~
principa:L resonator by means of a transrrri:;siary line:, ~tef'lex
lcl.ys tron;s represent one c:l.ass~ of slz~..l~ os~ :~1 l r~~ toz�s� ''her
theoreti~!~a1 formulae are tl~o~e from an earlier work (Ref, 1) a
.A.~.1 the formulae arQ slid for the symmetrical osc~~.la~tion
zonesU the oondit:ion of symmetry being expressed by,
Q ~ ~t~ ~ R ~) ~- Q
where ~'.l and ~2 are ''the resonant rva~relengths of #.he
auxi._liar�~,~ and the principal resonator., QB~ and QB~, arc
Card 1/~

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r. -,:~
~..
On the Theory cif Frequent~y Cha?,1 ~ t,I.r~~ ;~* 1 ~, ~~- T-:,I~('~ ,_ ,. _
t ~ l 1. A ill,/ ~.J CJ 1. r.~~ ~ 1 S ) ~ i 1 .. :j I i .~.
Lumino~hore.~
the tyke of ~r'~:roin~~>rt~l~~~.t;~i~.~r~ m~=-~ l,~~r~ i .~ttl tJ~,~ 1_ },~ .:,ha~~-
of the :f reauenc;;y c~L~arac, t,E,ri ,t1 ~~~ fI'he i~~~~ cJf� ~:.a.~~, Tl~~':.,i,-
flux modulations 1;~.11i^1:~ rs d.~ff'er->nt, 'iom .:~cc?~1 i;riit,iF-: ,.~
f`rec~uen.e.y c}~~3.r~.~C~r?3.'I.;;t].r:~ Ci~ ;t;1.1'lt~lll.::if11.S]~~ t}!~~'_'eCO^i-..
binations .}.aW~ f'r~.Jl~ ~}~;:h c,~I,:rE:,rj ;a,,E., ~~,,r:,r,~~z,,,t:~I} :1 ~~;~
~.
Wx,t;h othar ~'+YtyF:.~ (:).~` IT1CJt}l,t.l.%~ ~;11?Pi ,, '~;�'1F'. f'I'P`~:i1_ar~i'1t'~`~r ~ `? ;:. _.
t@x'1,,~1CS C)f ~ ;-~ ~ n 1 } t ,
(y }'{ L~f~ ~]!~'~ ~r.>'~1J }F; {.~.~. li:._' ~..% iJ ... _} t.i ~_c ~w ~7 t.- r~ Lid 1. ~%rl l`i i.. ~.,F~ ~ ~� i,
V U lI G U (.l\r ~ ~) ~ ~ L t~ r'~ t' '# i. t. .J ._ _. .. .1 .~. > y
~ I~ .~; i-Ci !.~t1~' }cl'. C?1. }i1ii11.'s'i(_~1i.. I'ILi _ C ~ d ,
tl.t?Ili S}1a6~' .7_tl t; }1 E' c~.t.I I~F17r�`~ Ot~1.i 1tr? �}, ,, YJ':~ _
2 .,~ ~~~ ~ rCJIL~~ ~ ~ri~
recomb2~rlat_ian ;~ak~~ cIst~_u.~ ~,~z.lf.itlE ~~}aot:~~x~�c:~:~7.stt.J::~~� T}io f'.r~F~c~zertc;~
character. i..~ , ~ ,~ ., to ~`-
f C" `"~ `~ } td'J.i 1. !- 11 f~ }1 J_ ;.~ C, aF--~,~~i�,;,.,r, ,
:~r
the :f re.gt~F~rt,;:~ ~ tza.r>-~c- +~,r r~r ~:>~r~ :; -,~~~,~ ,,: F>r.t1e~! t ~;.~~:

r, !
- - ~ ,-
c'~rli~. l..ialTllil:.~'SC=E'il~~t; ~-)Lt ~_~~iF' ~liF' .1. ~ ,.

_(.; f ('~?Ii-L~ ~~!'~_~~.
~Cia~ill'ltr '' I `1C"f; '1.~~-~' ! li P'i~_l(~~;~T'~':'-i ;;? O~ :~ ~>j.' .tl~';1~1'Li'Ii)1~li_
p 1 r'] 1. r~~.~ :~F,
Ht3 d1. (,:U~ ;E'.:~ a.l,It.r3T' ciZ'tC1 c~ ~,1 , f/r~iC!1i1:Jt ~.~JLr l~j ,,,, i
t~~I'1V(?s f~C~Z'f1111_ic3ci t;1~::~`T'~KJi!;r'; )f~ i ,i_~t~)i-'Yt~~~ ':i ,.'i ;r~ , .,~,
'j + }}
i.Jrmll.l[~s shn~~'d t huh r.i~G, t. t= !l.r_.~r~ ~ 1 L
~~ r
i 1 i i-. t,' 11~ ~.�"i- "%~
~`.i.._lr,~ C)~ ~)Y1~.J1,i}i'~:'.�:i? .:i~rer
the mode o
These con.dit~.oa~s a:~~e sat::i~:ied b~' morn?tror~s; by :~r~me
kl;yst,rons , including r eft Ex klys trans and by c ~~r t airy
other va~luesa Two met.hcyds of c;onnevti.ng the s~xpplemEn~=ax:~
resonator are distingui. shedo d.ir- pct ~:onneotion by a.
tranr~rnission. 1.:ine to the main wa~rity~ r.�ox2necticn in s~er�irs
to t)a~ loads The general equatiori9 written fox the present
c as e ~ is gi~ren in Eqs ($) and (9) ~ the paramet e:~�~s b ein;~
defined in Eqs (5), ~~) and �)~ then the electrical length
Caar'd2/4 of the transmission l~~n:~e is short, tine total width of the
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li L~/~J ~;/11
to-x~'wa,th
A~,2~~$fl~N,3 Ma~3.,veh~.~= p� ti. h F~`eQue~ ~~~~1
AUTHOR o ~.----~. - V ex'~Y ~ ~
he�ry of R.ad~of i~'x~`a'
The ~' ~a~edex-~-y ~~
f1TT ~'~ Load
~'BSOnatl.nS a 4~ysa}aikh ~~63~b'n~~~' (i155R)
Iz~restiy ~ s~,i,Ll?motor`' is
~Q~~tIOD~�C~~'o Vol ~, Nr' 3 9 PP ~;l~.ss of. � ~ ~ ~ ~~~+ ~, a
1.9~~ ~ ulcer' the us of u
a arti~ ta.or~. to ;~~.a"
o~eratx.�n of ~ addi ~, trar~;,nii~ ; toz1-tiTl~`~~
T.h~. d to whi�h, ~n` ~~~~~ ~d ~~ thf
OT o c onn ' ,
A13~TR.A �s~-der'e SUiia'~ r..~x" ~``' ~ mmetrioal ~ ~ mG.s~ ~.
~�.� tar'Y xe. mode is Y
en' AnY o ~ .Y
s'~'Pplem oscil7-at~ng ~�p~.os
Tlie Other ~-; ~.,~ ~ ~~ 1a~ wb~r, ~
1~.ne~ leot~d� width a.nr] Fi~tur
s net; band cif. Th>`:
y~fecfx~' ~' G ~,una~'~~ i~ a~-agram ~.ix,e,~it~
eleetroni t~~a.f simP- a t~.ned
jump" rE.;ented by> ~onnerted to the ~..,fun`tlon
be rep..... t , ~, where ex~E'ratO~
-~,an ar elemen ~q (1) n of the ~ c #,~anc e
a non,v~,~,ne desCr,Ued b~Y ,l,~stit, en~idu
oha~-~~ot~-~ c~.ectron~-~ o f the
opeex yto the oscz i~.,atidr~ of the
hate sta~~-1.itY
xef' ta,pn to the P .for. the ~~f f
~.W,fu-n'~ ~.j n ex'~..t nr';~.c~i~ ~~rilnt enan� e
~~nd the ator4 ~.~ ~) and f.ar the :in tt~e e sots' ~" I
ene~`
the S s Z~q = C
o f s t at, e ~- ~c~~h e ~" e u l
~ stut,iontions i~; ~~ (~ ~ g
r.~soi.lla
Card 1Jlf
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sov/58-~~-~.-8~1
Translation from: Referativnyy Zhurnal ~~iz;ika, 1959, Nr ~, p X18 (USSR)
T-~~: Methods for Determining the E~,uivalent Circuit Parameters of a Resonator
G~nnected 2nto an Arbitrary Section of the Transmissi~. Line
PERIODICAL: Tr, 7'a~anroask, radiotekhn n-ta, 1958, Vol 2, pp 55 - 0'2
~~~~
AHSTRACT: A method is
proposed for dete.rminir~ the parameters of the equivalent
circuit of a cavity resonator connected into an arbitrarily chosen
section of the transmission line, This method is ba.5ed on the taking
into account of the effect off' ~~upling with the non-resonating oscilla-
tions of the res,~nator,
Card 1/1
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I
Sr~~/58-5g--~~~.g
Translation Proms Referativnyy Zhurnal Fizika, 1959, Nr 5, p 150 (USSR,)
AUTHOR o Malyshev, V ~ A,,__
TITLES Analysis of the Time Course of the Excitan Photoeffect
`%
PER70DICALa Tr, Taganro~sk~ radiotekhn, in-ta, 1957, Vol 3, Nr 2, pp 117 - 127
ABSTRAC�Ts The author calculates the time course of the photoeffect f'or the
follo~ving mechanisms a crys+al is irradiated with 11ght corresponding
to the exciton absorption band; the exeitons approach thel metallo:td
vaoancies9 are annihilated, and create ~-centers; other exci�tons in
transit approach the F-centers and create pho~oeleetrons and meta.l7.oid
vacancies on account of their excitation energies, The author der~.ves
aprroximate expressions for the variation with time of the photocurrent
(irr relative units) for colored and uncolored crystals after the
inception of protract�d :irra~ii.a.tian, as well as after the discontinua.tior~
Card 1/2 of irradiation when the latter ha.r~ lasted a ~;:iven r~hort iri ~e~r~v~,.]. oi' t,imr~;'~ -
~I
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s/i 3361 /oao/oo~/ao1 /015
Production of tubes from semi-killed steel... AC54~A127
the nonvontionaJ. procasa piercing can ea.aily ba poxfarrn~~d at 1150 - 11 t30oC.
However, even when the temperaturF~s were aufficiontl.y high (1230 - 12hCoC) ,
the rejects amounted to 80, as a result of incorrect adjustment of the first
piercing stand. The hardness of the billet is riot uniform in its croas-
section (Fig. 2). The core is harder, than the external layers. The fail-
ure of the piercing testa could be oliminatE,d by mod.ifyin~ :~omc~ of the rol-
ling parameters. The inclination of the rolls in the first s~tcind ws,s re-
duced by 1�, reduction at the neck of the ^o11s was increased by 2.7 - 2.8f
and drawing out the nosepiece of the mandrp4 by 22 - 25~. By decreasing
the inclination angle of the working rolls, friction and pulling forces in-
creased tivhereas axial slip decreased. Aa a result of the increased reduc-
tion, the central parts were processed more thoroughly and piercing was
promoted. The above mentioned changes in rolling parameters decreased the
amount of non-piercable billets from 8% to 1.7~. Non-piercing of the bil-
lets can be entirely eliminated by raising the cropping of the top to 2 -
3f. A further cropping (3 - 4~) should be carried out for the 900 mm stand.
The quality of the tube surf ace with double-layer structure is ilatisfactory.,
The rate of flawless products increases, to 95 - 98jo. The mE~chanical proper-
ties of the tubes made of the test ,feel complios with (-UC I (COST) 8731-58
Card 3~~ ~~
J
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2?_312
f
5~133~C~1 ~ OOO~~J0~~OO1 ~G 1
Production of tubes from semi-killed ateel... AO54~A127
the metal which were in contact with the mold wall, were already crystallilr
ink and formed alow-carbon, sulfur- and phosphorus-free ~~immin~~; skin,
tivhile, at the same time the core of the ingot vas still liquid. Aluminum
kills the rimmin,~ metal of the core, while the rate of oxidation. can ~.~e con-
trolled by the amount of aluminum added, Provided dnaxid~~tion ~r~~as r,,zrried
out in the correct way, the ingot consi.3ts of a a :oft, blister-free rim-
avera e 12 - 20 mm thick ar~d b~ a ~~emi-killed cQrc YvitY:
mini skin, on an g
uniform liquation of carbon, sulfur and Phosphor, (not excecdin~; 130:--~ , in
vertical and transversal direction. The average rate of the risi.r~g of the
metal in the mold wad 0.28 - 0.32 m~~min. The 250 x 310 mrn and 2E}O x 310 rnm
blooms made of the test steel were put into the pusher-type furnace of t}~e
tube-rolling mill. The surface of the blooms is -remarkably clean, not di:~-
playing any of the usual. flays of killed steel. The blooms were rolled on
400 mm st�gnds, with the working rolls hav:.ng the follc~ving angles of incli-
nation: 8 - ~� for 168 x 6 mm tubes, 8 - 9� for 219 r. 7 - 8 mm and 7 - ~�
for 325 x 8 snnr tubes. The piercing tests sho~~ved that the test rrietal ,�ras
more stron~l,y affected by the changes in temperature thar. billets made of
killed steel. The test billets could not be pierced at 1190�C, tivhereas in
Card 2~~5 ~
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1
22312
5~133~61~000~00~'~001~G15
A074fA~~7
f~ ~ ~
AUTHORS: Qyks, G. ld., Doctor of T~ChI1~.C~~1. Scioncc~:~, Drofe.~eic,r;
Svetlit3kiy, Ye. A�, Eng�in~~er;
r
Sharadzenidze, S. A., En~,ineer,
K. K. , Engineer, and j~;t~.nd-
Lolua
,
~a~Y~_~.~.~~., Engineer;
~`-~.,~ - En ineer
tin, ~ ~~":.':~I~: , g
Production of tubes from semi-killed .~~~,eel with a dout;le-layer
TYTLE: crystalline structure
'�
PERIODICAL: c
Sta1' ;ono. ~., 1861 , 304 - 307
carried out on automat
d
l
s
o
ledusteelr~
~~
con-
the
1. TEXT: Tests were
in
s
l
bes from sArni-killed steel, instead of from the advt~ilt~~~E'~~ of
t
ti
u
ng
ventional process.. A metal vas required, incorpora
For this pupose rimming steel samelted in
both killed and rimming steels.
den
d
bl~ir
ot molds vrith w
'
in
t i
`, -
o enhearth
p a
u
o
f
g
n
gran ales
furnaces was cas
~ting the metal f1 ,
t
t;.3 ton ing erru}
~~ithout in
ots.
) rvero introduced during pouring in t:l~ ~critr,~.~.
of steep
11
0
t
Z5p - 100,
of the
C .
.
~r~
on
casting (the carbon-content varied corr~~.apordinf;;ly l~et;rcell
the outer 1~~;;'trs of
one
and O. z3o) . Aluminum ,eras added. Upon aching aluminzu:~,
Card 1~,~
x
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P.
USSR/C,enE,ral and Special. Zoolo~r -Trisects .
Abs Jour Ref Zhur -Biol., No 7, 195~~ 3051.1
Author : N~,lyshev, S.I.
Title The Ways and Conditions of the Evolution of Instincts ir:
Wasp-like Hyinenoptexa.
0rig Pub Tx. Vgea. entomc~l. o-va, 1956, ~5, 3-50�
Abstract ; The evolution of instincts of wasp-l:i.ke Hymenopttr~a passed
through. a number of stages; first (pompil.oid) w- charac-
terized by the paralysis of the prey and subsequent prepa-
ration of the dwelling; second (sphecoid) -- dur~.ng which
the building of the dwelling was f~911owed by the prepara-
tion of one gib prey specimen; third (crabroid) ,.- dii'f~-'-
rent from the second by the preparation of smaller Prey,
cought one at a time; the fourth (bembecoid) -- i~hc
:laying of an eAP ors ~~}1e ~'~-x~st prey anri providing :~o~~ ~,}~e
larva bit by bit; fif~l.h (moneduloid) -- the laylri4~ cif' et