SCIENTIFIC ABSTRACT VLASOV, A.D. - VLASOV, A.G.

• Document Type: CREST
• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R001860230005-6
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: March 14, 2001
• Sequence Number: 5
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

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Roscow. In--henerno-fizichezkly ln3t*t"t
Nakotoryye voprosy ek3;erlmentallnoy rlz.-ki; [st-rn-kl vYP. 2
(SO24 Probl*13 in Elperinental Pnysi:5; colie2tion or Articles.
Nr. 2) Mosco-. AtomIz4at. 1959. 123 p. 3,200 copies printed.
Sponsoring Agency: P.SPSR. Jwlnlsterstvo vyasheZo i orelnegi
apetsiallnogo obrazovanlya.
Ed.-. B.M. Stepanov, roctor of Physical and Mathematical SCj*nCt3. %,j
Pr'Dra$30r; Tech. FA.: S.M. Popova.
PURN4R! Tris collcct!.-n or Articles to intended for graduate
engineers And phyal-.1ste engaged in rj,e d-ibn wr ;,r,yz-4=-
Mboratory) spparatcs, and automatic and teleachanic ev;,-Ipmcnt.
COWRAGE: This collection of articles on experimental phyjIs wait
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AUTHOR: Vlasov, A.D. SOV/109-59-4-2-18/27
TITIE: Longitudinal Motion of Electrons and the Tolerances in
a Linear Accelerator (Prodollnoye dvizheni e
elektronov i dopuski v lineynom uskoritele
PE RIM ICAL: Radioteldinika i Elektronika, 1959, Vol 4, Nr 2,
pp 295-302 (USSR)
ABSTRACT:- The accelerator considered operates with travelling
waves at a waveleng+,h of 10 cm. The device is divided
into sections and consists of a cylindrical disc-loaded
waveguide. First the energy spectrum and the injection
conditions a-re considered. The longitudinal motion of
a particle carrying a charge e and having a velocity
V = Pe (where c is the velocity of light) in the field
of the travelling wave, having an amplitude E and a
phase velocity vp = Poe, is described by:
de = eE cos 9 dz,
dcp = 2A 1 15 = 2711 E;
Card 1/4 a-z X- (070 5- T-(Fo V&7-2~_ ~e
0

SOV/109-59-4-2-18/27
Longitudinal Motion of Electrons and the Tolerances in a Linear
Accelerator
where s is the enerbT of the particlet so is the rest
energy of the particle, A is the wavelength, z is the
longitudinal co-ordinate and (p is the phase of the
particle. By integrating Eq (1), an expression in the
form of Eq (2) is obtained, where ck is a constant
depending on the initial conditions. When the phase
velocity of the travelling wave is equal to the velocity
of light, Ecl (2) can be written as Eq (3). This is used
to plot the phase trajectories of the particles for
A = 0.625, Oo = 1, Po = 1 + 5 x 10-5 and for various
values of (~ . The injection7conditions for the system
can be expressed by Eq (6) where the values Of EH9 A
and-SH refer to the conditions at the input of a seNion
of the waveguide. The dependence of the output ener&y
on the injection conditions can be found by determining
the second integral of Eq (1). When 00 = 1,, the output
energy is expressed by Eq (7), where E denotes the
average value of the electric field. The energy spectrum
at the output can be expressed by Eq (8), where the
card 2/4 summa ion is taken over all the values of the function 9H-

SOV/109-59--4--2-18/27
longitudinal Motion of Blecturons and the Tolerances in a linear
Accelerator
The dependence of the spectral density on the output
energy is illustrated in Fig 2. From the above formulae
it is concluded that by means of the accelorator it is
possible to obtain comparatively narrow spectral It is
shown that at the wavelength of 10 cm and AH = 0.625,
the spread of the output energies does not exceed 1% for
more than two-.thirds of the total number of the injected
particles. However, the errors in the dimensions and the
operating parameters of the accelerator lead to a
reduction in the energy of the accelerated particles.
It is, therefore, of interest to determine the reduction
in the output energy due to the changes of the phase
velocity of the accelerating wave, temperature and the
dimensions of the waveguide. In analysing this problem
it is assumed that the phase velocity can be written
as vdp = (00 + P,)c. The phase velocities of the higher
harmonies of the accelerating field can be expressed
approx1mately as -v&n = ne. The changes of the amplitude
Card 3/4 of the accelerating field can be expressed~by a

SOV/109-59-4-2-18/2?
Longitudinal Motion of Electrons and the Tolerances in a Linear
Accelerator
coefficient (1 + P.-). Consequently, Eq (1) are written
as Eq (10) and (11). Partial solutions of these
equations are found and it is shown that these can be
employed to determine the tolerances of the accelerator
for the prescribed values of the phase velocity error
and the reduction of the output energy. The application
oe these formulae is illustrated by a numerical example.
Tlie author expresses his gratitude to E.L.Burshteyn for
his valuable remarks. There are 2 figures and
8 references of which 3 are Soviet and 5 English.
SUBhtTTTED: 16th May 1957
Card 4/4

66.361
2- SOV/120-59-5-4/46
AUTHORS: Burshteyn, E. L. and Vlasov, A.D.
TITLE: Design of a Klyst ron Buncher for an Electron Linear
Accelerator
PERIODICAL: Pribory i tekhni ka eksperimenta, 1959, Nr 5,
pp 26-28 (USSR)
ABSTRACT: It is well known that the energy resolution of electrons
accelerated by a linear accelerator can be improved by
using preliminary wave-guide or klystron bunchers. The
present paper is concerned with the choice of the
optimum character istics of klystron bunchers. Consider
an electron which leaves the injector with a kinetic
and e
energy W nters the gap of the buncher with a
i
phase 0. After passing through the gap the energy of
the electron will be W = W
(1 - m sin 0), where U is
the amplitude of i
the voltage applied to the gap,
is the
m = eU/W energy modulation coefficient and
i
the phase 9 of the electron relative to the accelerating
wave at the input of the accelerator is given by
(p = 0 - A sin 9. It follows that the relation between
Cardl/3 the energy W H a nd the phase (pH at the input into the
Ir

66361
SOV/120-59-5-4/46
Design of a Klystron Buncher for an Electron Linear Accelerator
accelerator is given by Eq (1) and this is shown by
curve 1 in Fig 1. The quantity A is the so-called
bunching parameter and is given by Eq (2), where
Ij is the distance from the buncher gap to the input
of the accelerator, W a is the electron rest energy
and % is the wave~_length. In the case of a linear
accelerator with a constant phase velocity c and a
constant amplitude EM of the accelerating field,
the electron energy W and phase (p is given by
Eq (3), where a = eE m %1W0 and 0 are the limiting
values of the phase y * Eq (3) is only approximate
but may be used by assuming that EM is the field
amplitude at the input to the accelerator. Curves 2
in Fig I represent lower parts of the phase trajectories
for different initial values of VH and W H It is
assumed that the accelerator is sufficiently long so
that the relative spread in the output ene ies is
determined by the spread in the values of I . The
relative spread of output energies does not exceed
Card2/3 q(q 4< 1) for those particles for which I-q,< lsinq~JK 1,

66361
SQVJ120-59-5-4/4
Design of a Klystron Buncher for an Electron J11near Atceleriaqor
i.e. for those points on curve 1 in Fig I which lie
between the phase trajectories 2a and 2b which
correspond to cos ~ � J -2q - The problem is then
reduced to the determination of the buncher parameters
and the value of the injection energy for which a
maximum number of particles is found between these two
limiting phase trajectories. Formulae are derived
which may be used to achieve this.
There are 1 figure and 2 references, I of which is
Soviet and 1 English.
SUBMITTED: August 4, 1958 L-K
Card 3/3

9-1300
AUTHOR: Vlasov, A. D.
TITL E' Oil
Corwept, loll
PE'RIODICAL: Radlotekhrilka 1 P6,I), Vcj I
pp
ABS)TRACT: The stabi,Jity of' of.ectron bearn.,5, culculatf--d t.)n the
a.",numption (if' the pve-,;enc-f! of boundary pal-ticles and
laminar movement of, L., 'allalyzed. It i~i shown
that this aidely accelptled :ippi-oach dock,; not alviay:; glve
correct arrwer.,.i, and in many ewie.; lead.,; t-c beams Gf
unstable structuve. The anaAy.1-1.s oi' clectron boams
with a con.~iderable ~;pac~~ chm-ge, and f'ocu~,-cd by jlonf,~-J-
tudirial. maLnetic fle~ld, io u-mally ba,,(,cl or, I.-he a.,3-~ujrip-
tion of I the pre-~ence of boundai~y particle:z;, arid ti-io
eqUatiOrl 01' MOIJ.01-1 C)C ItAic electron located or, the Outer,
sur-face (A' the beam i,., -2olvc.-d. The trajectoriet; of' the
Card 1/9 inner electrono are a.-,outrit"d to l*o1lo".1 the Olectz-D'i

On Brillouinto Elect,-, at / '('( ('(' 1 11
-),j
/I
Particle Conception "J,
v"'Ij uo Y (larflinar rl'ow). colicepi, of i-'hu
boulidary pin'tAck. k., Ulu, 01, I'h(-.
Bviltuitin 1-ut,evelice ;0, elld
a I id 1.-t w We] Y a ccepted by :;- Le I I I, I.,, t:' W1 I t I c fllo~l t, o 1,
the Invest,ijratiow, ave wti'll the equE1.11a.111m
conditions in tlie eleci-Xori Vlow, LL i.,
I;o in~wre the st.-Iabilily of the equilibrated beam
structure. A cylindrical coordinate syst.-em r,
-, the z-axis- coinciding with the axis of the symmetri-
cal beam io, tioed. A lonteit;iidinal magnotic field B zi
axially 3ymmetrical. focuoe.--, the The r~wliu:3
chavit,e:.; along, Uie z-axis are s Ir, w. Under the.se condi-
tions the radial movement. r)f* the elec',-on in i-1he 'heam
i:~ du~;cribed hy Eq. (1).
Carri 21~) 11
+ U.
111 '47"( .

On Brillouin's Electron Flows and Bouhdary 77778
Particle Conception SOV/109-~7-2-11-26
1 _ p2,
Here m = M m0 - rest mass of the electronj
e - electron charge; )Y = v/c ratio of electron
velocity to light velocity) t timej Pr - radial
force due to the space charge of the electron beam;
index "o" denotes initial conditions of' the variables.
I(r,r,, current through section with radius r.
The charge of the beam induces an electric and a mag-
netic field with components
Therefore
P, e (L-,. - v,bl,)
Card 3/9

On BrillouInts Electron Fl.ow.,i an(l lloun(lavy
C, og
Particle Conception
This expression is ;ubstituted Into (1),
f I. introduced and the slow chanf,-,e of' in is
mo
talcen Into consideration for tran.9forming (1) Into
d1p DI(P.P,) cp",
+ Ap (2~
where
B C (3)
4,0 2.m
If electrons are present which are on the Outside of
the beam the whole time 10 = PI- ) the movement of
each I-- described by the equation
'-'2Pr BI Cp,',
+ AVr = - + .1 ,
Pr Pr
Here T I sit ti full current of the beam.
Card 11/9 The current d(Jn-s -y irough the section of the beam,

On Brillouin's Electron Flows and Bouridary 77778
Particle Conception SOV/109--5-2-11/26
the longitudinal velocity v z and coefficients A, B, C
are assumed to be equal for all particles. As shown
,,0. Equation (11) proves that a
by (3) BI>O, C> U
radially limited beam 13 Possible only for A '*-0, for
.1
which condition, as proved by C. C. Wang (U.S. ref-
erence), the solution of' the boundary particle equation
In a periodic po,,,Itlve function with a period T
Pr ~ Pr MPr (t -1 - T),
fluctuating around the equilibrated value of radius
P,, which 1:3 determined by the biquadratic equation
+
Equation (6) is derived from for r - const.
Since certain deviations from the assume(] conditions
are Inevitable, tt 1s, necessary to consid, , the general
oolut.LGn oL' Eq. lopondlng, un two arblti-ary con-
stants. For 2tabll'A.~.: til' tht, beam ntructiire it 1:3
Card 5/9 required that the small- deviations of the Initial

On Brillouin I a Electron F' and 1?oundary 77'(113
Particle Conception SOVII 09-5 -2- -1. 111~20-
conditiona lead only to limited de-iiat,3no
particle trajectories from the asaurried. The cair '- ,-;hen
C 0 Is inve.,itigated, which takes place, e.9.., when
B --
0 and 0, the cathode is -:hlelded from the
focusing magnetic fleld, atol thu ele< troiw 1,~~avo the
cathode with zero azimuthal v(-Iocitl~ Equation (2)
becomes 11near
but the needed fzlcii.-~Ing field (ror gLven BI,
minimum; D_ -- B min - '-)m A/131/ej~,, (see (6) and
(3)). The general "0111tion of (-() 1.3
w h r- r e f- -,.T. _T second particular :jolution of
)Jrwavly hid-i.,-ni(lent of' TIF (5). Norntnally the
trajeetol-10-(j rij, are (,on.31-deved ao being
Card 6/9 similar to tht--, of the ou"'ev pavtlcle (5).,

On Brillouln's Electron Flows and Boundary 77778
Particle Conception SOV/109-5-2-ii/26
I.e., it Is C2 = 0 and 0 < Cl,-14 hrst and with 22-25 ml pure UO2Was
precipitated. At 2000C reduction proceeds more slowly is I.ess complete.
UO 2 I)roo'P'tates "' finely crystalline form (size 0.01 mm, lattice con-
stant 5.45-5-46)U30., somewhat wore coarsely crystalline at 200 0C
(0.01-0.2 mm). There are 2 figures and 1 table.
SUBMITTED: November 28, 1961
10ard 2/2

RAFALISKIY, R.P.; VLAS.OV, A.D.; NIKOLISKAYA, I.V.
Possibility for the synchronous transport of Uv' and S by hydrothermal
solutions (based on experimental data). Dokl. AN SSSR 151 no.2:
432-434 J1 163. (MIRA 16:7)
1. Predstavleno akademikom D.S.Korzhinskim.
(Uranium) (Sulfur)
(Geochemistry)

BONDAREV, B.I.; VLASOV, A.D. ---
Self-consistent particle distribution and limit current in a
linear accelerator. Atom. energ. 19 no.5:423-428 N 165.
(MIRA 18:12)

VLASOVY A.D.
c.f
*-~rl "' a
. 1. -
chargn, RaCticit-:4.1, 1 546 Ag 1650
(Ml,U :8:8)

s
T hoe o 11-gar a-colara*,ars llnayriYW~, uskorl!-eley) M,~,scow, Atcmizodat,
TOPT' 'A ,u part"le a-c-.1eretor, hl-li energy at~,,olorator, iina&r ELccalarator, at.-
~z-l 9er p - p ry -~n
RUT. 75- 7"'? Mi
at--zi

ACCE-S.31ION NR *15013556
intended for a c, if-Int I P'Le anti Rng!
,ABLE CTF (abridged):
?reface 3
Conventionai spahcls - 4
introduction - 7
Ch. I. Accelerating aysteme and wTion equatione - 17
Ch. U. Longitudinal moticn - 44
Ch. 111. Defocusing forces and focuBi-ng "thods - 103
tCh. N. Qmdrupole fccuzing - lYt
Ch. T. Alternating gradient focusing by accelerating field - 208
Ch. VT. Focusing by means of lonffltudinal magnetic field 232
Ch. Vll . Grid and foil focuslag 24b
h Ii T TThr
_~J I
ail- _iz?._;'t'
Appondix 214 A
Bibl-iography - 301
Card 2/3

VLASOV, Aleksandr Daniloviclip dokLor Lekim. nata. ,v,);,Ytajy 5.L,,
-1-FO-1-11-1--l- :- - ---- ...... j
[Theory of linear accelerators] Teoriia lineinykh U3kori-
telei. Moskva, Atom.lzdut, 1965. 306 p. (MIRA 1814)

L 1525o-65 --EC (b 2 2/--'--
3 ~7 D, A.,~ D (a D t
ACCESS ION MIR : A P5 0A 112 (-12 1(-f"-? 1 - 2 314/124
AUTHOR: Vla-cov, A. D.
TITLE: Theory of nonlaminar electron flow focussed by a magnetic field
SOURCE: Radiotekhnika i elektronika, v. 9, no. 7, 1964, 123.4-1245
TOPIC TAGS: longitudinal magnetic field, particle motion, electron flow
ABSTRACT: The nonlaminar structure of an axially symetric electron flov
focussed by a longitudinal magretic field is studied. The upper and lover
lim-Its are found for the focusaing fl-ld. Tbe vej! itna,,al fact that th~
requ',-ed field is alvays greater --ha' prcdl-t-d by the laminar trer-?ry
of ~ir'!Iouln 1G 1F :,i1-1!---:-. rr f~~-- a 6 " no,1 e
for an Lna-?-PenPd ~-a~hrAe,
r pe Qg
on vhether or aot %h-e the a-x4z; of the flow. Equat Iona
are derived for Dzrtl~71,e
rotiticrishIp betwef~n -harge den-
qi'~-- riltilrlxbut ',,on urd for varloui,4 tra-
Je--!-Orlea. 111..~~;, -rlw. ar,. ruis:
~~ f,~rmu.IB6.
Card 112

L 15250-65
ACCESSION 11R: AP5001202
ASSOCIATION: none
SUBMITTED: 22Apr63
EKC'L: 00 SUB CODE: NP,EK

NO REF SOV: 003
OTIMR: 003
JPRS
Card 2/2

-Vi4sovp A.D.p doktor tekhn. nauk (Moskva)
Eminent Soviet radiotechnologist and electronics expert; 70th
birthday of Academician A.L. Mints. Friroda 54 no.ljl20-l2l
Ja 165. (MIRA 18t2)

,;II.SOV ) A.D.
Syste,..i 130-, - Nu2CC;3 - C02 - Tl;,'C" - a-u elevated
4. - I (
.1 1 1 1 0 ~rr
I
and pressures. Zhur. neor~,. ~,*,jrl. Q, ',, -1
-11- -- - I

VIASOV. A.F.
OrVanization of service given by the North Caucasian
Hydrometeorological Administration to agricultural administrations.
Meteor. i gidrol. no-4:40-41 Ap 163. (MIRA 16-5)
1. Severo-Kavkazskoye Upravleniye gidrometeorologicheskoy
sluzhby.
(Caucasus, Northern-Hydrometeorology)(Caucasue, Northern,-Agriculture)

MALMOVA, V.F.; RATOVA, T.M., starshly inzh.-klimatolog; MORDUKHAY-BOLTOYSCIT,
D.D.;.,-VMSOT, A.F., otv.red.; NEDOSEVINA, T.G., red.; SMGEYgv,
A.N., tekhn.red.
(Agroclimatic manual for the Kabordino-Balker A.S.S.R.] Agroklima-
ticheakii spravochnik po Kabordino-Balkerskoi ASSR. Leningrad.
Gidrometeor.izd-vo, 1960. 135 P. (mIRA 14:4)
1. Russia (1923- U.S.S.R.) Glavnoye upravleniye gidrometeorolo-
gichaskoy aluzhby. Severo-Kavkazskoye upravleniye. 2. Rostovskays
gidrometeorologicheskaya observatoriya (for Malikovs, Batovs,
Mordukhay-Boltovskiy). 3. ITachallnik otdola agrometeorologii
Rostovskoy gidrometeorologicheakoy observatorii (for Malikova).
4. Nachallnik otdela gidrologii Rostovskoy gidrometeorologicheakoy
obaervatorii (for Mordukhay-Boltovokly).
(Kabardino-BalkBr A.S.S.R.-Crope, and climate)

VLASOV, A.F
Results achieved b7 h7drometeorological stations in supplying collec-
tive and state farms with agrometeorological information. Meteor.
i gidrol. no.10:38-40 0 160. (MIRA 13:10)
(Meteorology, Agricultural)

VLASOV) A.Fe
Increasing the flOwabilitY Of mOlding mixtures b7 modified suspension.
Lit.prolzv. no.4:5-6 Ap 163. (14IIW 16:4)
(Sand# Foundry-Additives)

GRUOVSM, 0.1., prof.# retsenze~t; ROSSIYANOVq D.D.9 inzb,j
retBenzent; BROKLUt M.F,*, kand. tekhn, naukp red.; SMIRNOVA# O.V.#
tekbn, red.
[Removing dust and chips in macpInIn brittle materials) Udalenie Pyli
i struzhki pri obrabotke kbrup)4.kh materialovp Moskvaq Goa. naucbno-
tekbn. izd-vo mashinostroit. 3it-ry, 1961. 130 p. (MIU 140)
(Metal cutting)

AUTHORS: Vikhoreva, T.A., and Vlasov, A.F., Engineers 128-58-4-11/18
TITLE: Experience 7ith Exothermal ly-Heat ed Feeding Heads (Opyt prime-
neniya pribyley s e,kzotermicheskim obogrevorr)
PERIODICAL: Liteynoye Proizvodstvo, 1958, No. 4, pp 25-26 (usm)
ABSTRACT: The article gives information on a new exothermal compound
for heating feeding heads of steel castings which has reduced
the metal waste by 50i'. and also greatly reduced the number of
rejects. Its composition, in weight percentage is: powder
aluminum 10/~, 75-percent ferrosilicon 13~c, iron scale 62-i,,
refractory clay powder Sp fire clay V-. Addition of 3-51,
3ulphite lye and li, water is made to increase the strength
of the compound in dry conditions Recommendations are given
concerning the diLlensions and weight of feeding heads,and the
granulation of exothermal compound components, The compound
is considerably cheaper than the ordinary exothermal compounds
containing more aluminium powder, the burning reaction in the
process of pouring is quiet, the remains of the compound
nz,rtly float to the metal ourface in feeding heads and form
a readily removable slag. in illustration shows a casting
Uard 112 with ordinary feedinC heads and one which was exothermally

Experience 'Vith Fxo thermal 1y- Hea t ed Feeding Heads 128-518-4-11/18
heated by using the above mentioned compound.
There are 2 figures.
AVAILABLE: Library of Congress
Card 212 1. Steel tastings-Test methods 2. Steel castings-Test results
A

-- -----
VWOV, -A F Nl"~
741-41
.V81
Tekhnika Bezopasnosti Fri Rabote na Metallorezhushchikh Stankakh
(Safety Techniques for Work With Metal-cutting Yachine Toole) Moskva,
ma8hgISO 1951.
199 P. illus.I diagra., tables.
Literatura: P. 193- (194)

- NY/ -I A -, , , /I ~ I% it .
UfXgl, A. F.
Tel6inika bpzop~,sjnooti prI. obrabot'-k3 I-Ietmilov rozan-len L-Safety tlechnirrws
Aal cuttLnzj. Pod m-d. A. V. Pankina,. iNoskira. Proflzdat, 1..~12 .
in :Tie 1~ 72 p.
SO: ',,IoathLr L~gt gf R3aggi:iji Agcoa3If-)U. Vol. 6 ',,o. 7 October 1953

1. ~TE, I'~5ZA-EV-3 E. G. ) VUSOV. A.' F, ~ GFUXIIEV, L. N.
2. USM (600)
4. Lathes - .1afety Appliances
7. Safety devices for lathes. Stan. i Instr. 24, No. 2, 1953.
9. Monthly List of Russian Accessions, Library of Congress, ~:uy- 1953. Unclassified.

V/,,q6ov,hl&q,dlr
VIASOT, AlAkq&ndr Yilippovich; DWISOTA, I., redaktor; KrRSANOVA, N.,
takh cheskiy 'redaktor
[Safety engineering for metal cutting] Tekhnika bezop&snosti pri
ebraboike metallov rezanism. Izd. 2-oa (Moskv&3 lzd-ve VTsSPS Pro-
fizdat, 1954. 74 p. (KM 80)
(Safety engineering for metal cutting)

VLASOV;MAIgj r Filippovich; PANKIN$ A.B., professor, doktor takhnIcheakikh
re4ak-tor-, IMNISOVA, I.S., redaktor; RAKOV, S.I., takhnichsakiy
" r
redt-ktor
[Safety techniques in high-speed metal grinding] Tekhalka bezopasno-
sti pri skorostnom tochenii metallov. Pod red, A.V.Pankina. [Moskva]
Iscl-vo VTsSPS Profisdat, 1954. 124 p. (ML'RA 8:3)
(Metal industries-Safety measures)

VIASOV, AleksapdrF11IRRo VESNLKIIIA, A.A., redaktor; KIRSAIIOVA, N.A.,
_i~~j ~ .
DUM&F
[Principles of safety engineering] Ganovy takhniki bazopasmosti.
(Koakva] Izd-vo VTaSPS Profizdat, 1956. 106 p. (HLRA 10:3)
- (AccidentB--Provant ion)

V'LA,SbV --A -tFa----
ZLOBINSKIY, B.H.; TRUOIANOV. A.A., doktor takhnichaskikh nauk, professor,
retsenzent; KRUKOVSKIT, V.A., dotsent, retsanzent; TLAWY, A.F..
Inzhaner, retseA!pnt; VINOGWSKIT, N.T., dotsent,
[Elements of safety technique] 09novy takhnlki besopasnosti. Moskva,
Goo. nauchno-takhn. lzd-vo mashinoetrolt. i sudoetroit. lit-ry, 1954.
212 p. (KWA 7:7)
(Industrial safety)

VL&SOV, Aleksandr Fill ovich; URYKOVA, G.I., redaktor Izdatelletva;
- __ suo.~ -,.-W
, T.Y., tekhnicheskiy,redaktor
[Safety measures when operating machine tools] Tekhnika bezopasnosti
pri rabote na metallorezhushchikh gtankakh. Izd. 2-oa, perer.
Moskva. Goo.nauchno-tekhn. izd-vo mashinostroit. lit-ry. 1956. 212 p.
MRA 9:8)
(Machine tools--Safety appliances)

RAKITI21, G.A.; UA�PX*jj?x; GLAGOLZVA. T.A., kandidat tekhnicheakikh nauk;
KMMIKOVA,V.I., kandidat teLchnichookikh nauk; KUZANTSM . Te.l.;
KUCMMUK, Y.Y., kandidat tokhnichookikh nauk; P=GPOP07. I.P.; JXO-
TSTANOT, L.Y., professor; DUBOVA, I.B., redaktor; KMAKOVA, N.A.,
takhnichookiy radaktor.
[Labor protection] Okhrana truda. Isd. 2-os, Isr, Hooky& Izd-vo
VTsSPS Profizdmkt, 1956. 278 p. (MLIRA 9:5)
l.Moscow. Moskavskaya vyeahaya shkola profdvizhenlya. 2.Chlen-kor-
respondent Akademil meditainskikh nauk (for KhotoYanov).
(MUSTRIAL HYGMM) (BDUMIAL SAYNX)

JU BARYKOVA, G.I., roduktor izdatelletva;
'9UO_WV_A,_II.'Y., takhnichaskiy redaktor
[Safety measures when operating machine tools] Tekhnika bezopasnosti
pri rabote na metallorezhushchikh stankakh. Izd. 2-oe, perer.
Moskva. Goo.nauchno-takhn. izd-vo mashinostrott. lit-ry, 1956. 212 p.
(KLRA 9:8)
(Machine tools--Safety appliances)

jiyh-,,.DENISOVA, I.S., red.; GOLICHENKOVA, A.A.,
VLASOV, Alekeendr Filipj?
.& ~_A .
21
(Safety techniques in metal machining] Tekhnika bezopasnosti
pri obrabotka metallov rezaniem. Izd.3., perer. Moskva. Izd-vo
VTsSPS Profizdat, 1958. 92 p. (MIRA 13:1)
(Metal cutting-Safety measures)

e-TIANV# A34mdr-nUppovicb; DENISOVAp I.S., redo; KCROWVAp N.D.)
-4itwows
hadnaftlo of sOety enjimering] Oonmy UkhAiki
.II mopsmAio lsd*2,pp peraro Momknq lad-owo Protisdat
IWo 207 Timustrial sOety) (0 15 t 5)

VL-AS'OV, A.F.
~--
Conducting agrameteorological observations from a helicopter. -
Meteor. i gidrol. no.1:50-52 Ja 165. (KIPA 1822)
1. Severo-.Kavkazsk.:)ye upravlenlye gidrometeorologicheskoy sluzhby.

VLASOVI Aleksey Fedorovich; MIARVIK, Yovf,,,eniy Yofimovich; BORIN,
--Ivah-Sergi~e Vi. ch j KONONOV, D.R., red.
[Drying foundry molds and cores by means of infrared gas
burners) Sushka liteirykh form i sterzhnei gazovymi go-
relkami infrakrasnogo izIucheniia. Leningrad, 1964. 20 p.
(MM4 17: 11)

VLASOV, A.F.
Methods of improvIng the shakecl~ztl c.f water glaEs mixtureF.
Lit. proizv. 5:36-38 14Y '64. (!J 7 F,&. I a ; I '

VLASOV A.F., kand.tekhn.nauk
-, J~.,
Pneumatic removal of chips and dust. Mashinostroitall
no.8:33-38 Ag 165. (MIRA .18:U)

1".
L JV oxis of a stral:,iit --,l
of Lenin -Itzlte U iile-1-1-i (Dissell'atior. 1''Jr tl~ie
:je,,.ree of Lo.3tor of sicoc-liemical Sicience;.
10, 22 October 1951,i. ;~:.-)scow
SO: Kriizlinava Letmis" lio.

1 "702
-,-
,i
J0;
NM
, G.W. ad
u
,
P
AUMORS I Gr-o..kly. T.L., L-k'.Yaho~.
sirotonko_ I.Q.
TIMB i - ~S_aad Conference In Gas
91matronics
PZRIODICAL; RdIat.k--- 1 1959. VOL 4. Xr a.
vv L339 - 1358 (USSR)
Ac. So USSR the
.d
by th:
ARSTRWT3 The cof.ramc.f --- -r4.AI
L
~or.ity.
.
:.
.
Malstry of Higher gd-c .tt .4 Ho .. ,At. U
j
It ma. op".4 by the chairman Of the orgealsing committee
Azads,sioten. Daring the P164&" Sesston
bar of *~rwoy papers war.
;.:.Tpaper on mProduction or Ultra-high
A urway of the Optical .ttk.d of measurements was giwon
la the paparv, by V.A. F.brik..t ad 5.19. Fri-h.
S. Drawn of %be Massachusetts Inatit.t. of Technology
gave . sor,.y of the bjXb-fr.q....y methods of the lav..ti-

~ry &A4 noft;stat onary plamma (see p 12kk
I.. ti. I
to
or
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g
l
e
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:
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thi
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read paper entitled
th
.
-~.
N
F.
C.rdL/15
Hlio.T- or a,, D!~. Atomic C-lli8i-a---
! I x
with
l
aglase ntay Processes
As I Ga.".
a
o
A paper by To. Bodarou (Ruxsuia) dealt with "The Role of
Kinetics or louse.
conzid:r*4 the in4tial stages Of the
.Xopmezxt of p~ks (c roua-lead4r, main Channel and the
f-I ch...2.0_
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Th. ."b-.1" Of the breakdown of . biSh-so.- gap we.
elucidat*4 in a paper by W.L. Granow."y.
L. TonkA (US expound*4 a theory or the motion of

slactrons in vatic trap (-** p L516 of this Journal).
car
Acmdamiclan A_ Romp. CZAstem Germany) described a number
of experiments on non-stationary plasma coud,ucted by
bIms.lf.
X. stemboax Germany) Cows a C.asralis.4 theory of

A action..
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Th. f.LiaiAg Papers were read in this actiong

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~
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I- Rarlfl.d
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To- K- T66-1- with V-A,_A.LkUdjn93L
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`C~~* &Ad Loss of ZI-ctrana During
fast A oss of carbon and Hydrogoa with the X.1vaul.s of
t
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Of Rydrogs, Dwring Callisio" In Gas*.
.1-2-Al". -ad Y1.T__1a1Ar2_xAx_- "C.pt-.
Of LleCtro" 1A M&Iticharge Laos in X.art G-.*-.
1. - "Zxperimental Xnvostia&tjoA of %he
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grrwotL~. zz Lt.tL.0 C--actio" of the
:
L
f Pot .. I-
d A.,S..-.
C-r43/19 and A.M. R.j.1t. of the
InVestization of the optical F-ti... of the zZoitotion
BoAder^ X.g.tLv. Syet-..
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:
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and was de-ote4 to the problems If th. electrical break.
down in r-L f& ^,.
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:4 g
papers . r.
rc 4 1
o
L
j
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G.r.- and Yu,A-,H*~jtc
s"y__ *CloCtrostatto
_
Control of the Igultion of Gla-d-th.rg. Tb..'j...
p1271, of th aJ.urual)-
S.-P,ItsM at &I. war* COuc*ruod with the b-kd.wa,
;V
L
. high-wOlt&1* m-1--Y 1"t1fL,r (- p 1278 of the
Journal
of th h
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- Me- -1 Is- Of
mas H'.. A

S1048 iP924/008/01
B012~21o67
AUTHORS: Vlasov, A. G., Voroblyev, A. A., Kislov, A. N.,
Meshc7a'r'ya`75`v, R. P.
TITLE: Investigation of the Losses in Electrons Due to
Scattering in the Residual Gas in the Accelerating
071amb
PERIODICAL: Izveatiya Akademii nauk SSSR. Seriya fizicheskaya, 19
Vol. 24, No. 8, pp. 1006-1012
TEXT: In the present paper the theoretical calculations of the losses
in accelerated particles due to sfi.Ltering in the residual gas were
experimentally examined. A suggestion is made for calculating these
losses. First, only the definite results of calculations according to
the methods by N. M. Blachman and E. D. Courant (Refs. 5,6), J. M.
Greenberg and T. H. Berlin (Refs. 7,8) and A. N. Matveyev (Refs. 9,10)
are studied and compared in a Table. This comparison shows that the
various methods lead to different results. The control method and the
Card 1/3

Investigation of the Losses in Electrons S/04f ?08~0924/008/016/017
Due to Scattering in the Residual Gas in the B012)3zel
B067
Accelerating Chamber
experimental apparatus are then described' Fig. 1 shows the measuring
block diagram. The results of measurements are given and aompared with
the results of theoretical calculations. In conclusion the following
is stated: character and quantitative comparison of the curves shown
in Fig. 6 indicate that the losses in electrons due to scattering in the
residual gas can be calculated according to the method of Greenberg and
Berlin as well as according to that of Matveyev with sufficient accuracy
since the results differ only by 1.5 -* 1.7 times from one another.
According to the method of Blachman an~ Courant the losses in protons
due to scattering in the gas may be estimated, whereas for the electrons
the values obtained by this method are too low. The sufficient agreement
between the experimental and the theoretical results also confirm the
correctness of the method of measurement chosen. V. G. Shestakov
assisted in the measurements. The collaborators of the NII TPI and FTF
assisted the authors in this work. There are 6 figures, 1 table, and
15 references: 6 Soviet and 7 British.
Card 2/3

82839
Investigation of the Losses in Electrons S/048/60/024/008/016/017
Due to Scattering in the Residual Gas in the BO12/B067
Accelerating Chamber x
ASSOCIATION: Nauchno-issledovatel'skiy institut pri Tomskom
politekhnicheskom institute im. S. M. Kirova (Scientific
Research Institute at the Tomsk Polytechnical Institute
imeni S. M. Kirov
Card 3/3

89694
S/139/61/000/001/002/018
EO32/E5i4
AUTHOR: Vlasov, A.Gi
TITLE: On the Calculation of Losses of Accelerated Particles
due to Scattering by the Residual Gas
PERIODICAL: Izvestiya vysshikh uchebnykh zavedeniy, Fizika,
1961, No.1, pp.20-23
TEXT: N. M. Blachman and E. D. Courant (Ref.1), J. M.Greenber
,and T. H. Berlin (Ref.2), A. N. Matveyev (Ref-3) and others have
~kt,alculated accelerated particle losses due to scattering by the
~11 residual gas in the accelerator chamber. The probability that
lafter scatt ering a particle will remain in the chamber is given by

j0
).2
2 e

where j are the Bessel functions, is the a-th root
and J
0 ,
Card 1/6

89694
S1130AI61100010011002lOi8
On the Calculation of Losses ... E032/E514
of the BesBel function 0, B0 is the initial amplitude of
betatron oscillations, b is the linear dimension of the chamber
i
n the direction under consideration and is the factor
describing multiple scattering. The particle losses are determined
(in relative units) from the formula:
(2)
The above expressions take into account elastic multiple scattering
only, i-, can be determined from the Rutherford cross-section for
elastic scattering, obtained taking the Born approximation into
account. E. D. Courant (Ref.6) has shown that *the use of the Born
approximation may lead to an over-estimation of the cross-section
and has used the elastic cross-section obtained by G. Moliere
(Ref-7) to calculate n- Moreover, Courant has replaced the
maximum scattering angle 0max by 9.1. which is given by
el b (3)
11 (1+a;172
0
Card 2/6

S/139/61/000/001/002/018
E032/E5i4
On the Calculation of Losses .....
In this expression x n for axial oscillations and x = 1 n for
radial oscillations, where n is the magnetic field index, R is
the radius of the equilibrium orbit in centimetres and 0
a = L/21f R and is the ratio of the length of the straight line
0 1
sections to the length of the curvilinear sections. The express on,
,...for then reads
70 N R3 Z2 I (I +E)2
a e - -a - (4)
4%bl Tie V
where 1..2 eM (1 + 3.33 tP21/2. z a is the
in 1 "l 137 min
minimum scattering angle, N is the number of atoms per cc in the
chamber, T is the injection energy in eV, Z is the atomic number
of the resiLal gas and eV is the energy communicated to the particle
per revolution in electron volts. The present author points out
that the use of the Moliere (Ref-7) cross-section complicates the
Card 3/6

89694
S/139/61/000/001/002/018
On the Calculation of Losseso, ... E032/E514
matter very considerably. For this reason the present author has
used the cross-section obtained by Mott (Refs. 9 and 10) on the
basis of the Thomas-Fermi statistical model. On this approach, 1
is given by
2 3 2 4 2
N R Z e (1+0 0
0 1
1n (6)
712 2 e
2mb T e V min
Numerical calculations have shown that the values of calculated
from Eq1.(6) differ by only 3 to 5% from*. those: -,obtained Xrom',I.
Courantaformula (Eq.4). On the other hand, calculations based on
Eq.(6) are very much simpler. It follows that in order to
calculate particle losses by the Blachman-Courant method, it is
convenient to use the cross-section obtained by Mott and to
calculate n from Eq.(6). The present author reports detailed
numerical data for particle losses in the following accelerators:
proton-synchrotron of the Joint Institute for ~'uclear Studies
(Dubna, USSR), the c6smotron (Brookhaven, USA). proton-synchrotron
of the Birmingham University, synchrotron of the California
Card 4^

89694
On the Calculation of Losses* ....
S/139/61/000/001/002/ol8
E032/E514
University (Pasadena, USA), Berkeley synchrotron (USA), and the
betatron of the Tomsk Scientific Research Institute (USSR). It is
shown that losses due to radial oscillations in electron accelerators
are comparable with those due to axial oscillations, while for
proton accelerators they are considerably smaller, since the radial
dimension of the chamber in the case of proton accelerators is 3 to
4 times larger than the vertical dimension. It is essential to
take into account radial oscillations in the case of the electron
accelerators. The pressure in the vacuum chamber should normally
be chosen so that particle losses due to scattering by residual gas
should not exceed 10 to 15%. The total losses calculated by the
Blachman-Courant method, modified as indicated above, differ from
the experimental results by not more than 30%. It follows that for
engineering purposes the above method is quite adequate.
Acknowledgments are expressed to Doctor Professor A. A. Voroblyev
for discussions and valuable advice. There are 2 tables and
11 references: 4 Soviet, 7 non-Soviet.
ASSOCIATION: NII pri Tomskom politeklinicheskom institute imeni
S.M.Kirova (Scientific Remearch Institute of the Tomsk
Card 5/6 Polytechnical Institute imeni S. M. Kirov)

On the Calculation of Losses.. ...
SUBMITTED:
February 15, 1960
89694
S/139/61/000/001/002/018
E032/E5i4
Card 6/6

22784
B104/B205
AUTHORi
TITLEs Effect of pressure in a vacuum chamber on the radiation
intensity of accelerators
PERIODICALt Zhurnal tekhnicheskoy fiziki, v. 31, no- 5, 1961, 03-615
TEXTs Experiments with a betatron having a radiant energy of 15-25 Mev,
performed at the Tomskiy politekhnicheskiy institut (Tomgk Polytechnic
Institute), have shown that, at pressures of (1 - 2).10- mm. Hg, emission
is virtually lacking, intensity increases considerably with a pressure
drop to (3 - 5)-10- mm Hg, and that intensity does not increase very
much with further decrease of pressure. The parameters of the accelerator
are listed in the accompanying table. For a smooth operation of the
accelerator, a pressure of (2 _ 4)-10-6 mm. Hg is required; further im-
provement of the vacuum is superfluous. An increase of the injection
energy raises the radiation intensity at one and the same pressure. The
lose of electrons due to scattering by molecules and atoms of the
residual gas in the chamber of the betatron at 15-25 Mev was calculated.
Card 1/4
8/057/61/031/005/015/020

22784
S/057/61/031/005/015/020
Effect of pressure in a ... B104/B205
The methods of calculation, originally intended for the calculation of
proton losses, were taken from a paper by Blachman et al, (Phys.Rev.,
JA, 140, 1948; 11, 305, 1949). In calculating the electron losses the
author had to take account of both elastic and inelastic collisions.
Furthermore, radial and axial oscillations have been considered.
Theoretical and experimental values are intercompared in Fig. 2 and were
found to be in good agreement. Summing up, it is noted that every
accelerator exhibits a critical pressure at which its emission will
vanish. It is advisable to evacuate the chamber of the accelerator down
to a certain pressure limit, since a lower vacuum wguld be useless. For
the betatron in question, this value is (2 - 3)-10- mm. Hg. The
theoretically calculated losses amount to 6-8% but the experimental ones
are somewhat higher. This is due to factors that have not been taken
into account, such as disturbances of the magnetic field, initial spread
on injection, etc. Doctor A. A. Voroblyev is thanked for a discussion,
and Engineers R. P. Meshcheryakov and G. M. Tsyb for assistance in ex-
periments. There are 2 figures, 1 table, and 12 references' 5 Soviet-
bloc and 7 non-Soviet-bloc. The two references to English-language
publications read as followas E. Courant, Rev.Sci.Instr., Z1, 836, 1953;
Card 2/4

8h
Effect of press ure in a... V05 611031100510151020
B104 B205
Mullett, L.B., A E.R.. E.I'~P/Ro ?072, 195'9.
SUBMITTEDs May 26, 1960
00
'Legend to Fig. 21 Theoretical
dependence of' electron loss-es AS
on scattering by. the residual
e-
-gas in the cham&r-6V-the
betatron.
:~z
0. 4
40.1
W 80,F a/ Al OJ as Me, 11,7
M*Im cm
Card 3/4

VLASOV, A.G.; PONOMAREV, V.P.; SHIVYRTAWV, M.T.; SHCHENIN, P.M.
Vacuum systems for electron accelerators. Izv. TPI
122:99-107 '62. (MIRA 17:9)

VLASOV, A.G., SHS41'11YUK, A.I.
Theoretical invest.1gation of tho poBBibillty of applylnp the m,,tk,~,d
of differential therml analyalii to the quantitative aLudy of the
Cry3tallization process. Stekloobr. sost. no.1:116-119 163.
(MIRA -17520)

S1058163100010011101311-10
ib~'2/Aioi
MFMOR: Vlasov, A. G., Kislov, A. N., Moshcheryakov, R. P.
i,nix.': Apparatus for measuring short-life Isometric-transitions.
PERIODICAL-, Referativnyy zhurnal, Fizika, no. 1, 1963, 37, abstract 'IA353
(In collectiont "Elektron. uskoriteli", Tomsk, Tom6kiy un-t, 1961,
P88 - 291)
TEYT: Apparatus for measuring short-life Isometric transitions is-described
The measurements were carried out on a betatron of 25 MeV maximum energy. The
apparatus comprised a cutting-off circuit which permitted also the control of the
maximum energy of bretnsstrahlung and the prevention of the error,due to osailla-
tions of the radiation intensity, a scintillation spectrometer operating with a
pulse supply, an amplitude analyzer and a 16-nhannel time analyzer. The duration.
of the cut-off was 3 Usec.
K. Aglintsev
[Abstra'ctpr's note- Complete translation)
Car~(j 1/1

L 578~0-65 EPA( w)-2/r~WV r-V~74T( b `,IF" A( r: E- I' P( t
NR: ~"4 X'C
yeyt -.Tenanlye. 3-.,:cLny-y I~orri, Abs. qA46
,kLM.--'CA- V'--a5ov, A. G.; Ponomarev, V. P.
6
TTME: ~7si-ng the 'titanium pumps for exhausting betatron chambers
CI7ED .-URCE. Sb. Elektron. uskoriteli. M., V,,,-ssh. Oikola, 11?6-', 386-30'
TOP-~ :A.33: titanium pump, high vacuum pump, betatron chamber
TRP-ISLATION: Tlne widely-used method rbtalnng hiall vqc~.~.~--i ~n lip
A
X: La ---vac InIL succeelec ry a 7 a
C.rd

7 c 7~ 2; 5
ACCES51011 NR.- A-R4049,406
starter that cons ists of a Uungs'-e--. 7-n -,P~ 7i~ v- -. c-, a
carrying wire is wou-nd; the sta-rter reduces 'he pressure from 1~;-P
I llec
T'hP ara.-et.ers are: cathcde currer.' , 12-15 7 c, - tor current ma
"Aze !--S vj ccllec' or voltage 1200 T~l r.1;--nin
'ir. ~L- e mad e j, F, - A*.' a
~,e ta on. A "a;~,
a' a g 7 a~m I-r meaF-;rlnj-, i~a3
r a e 3~;
SM CODE - HP KNOLt GO
Carcl 2 12

VLASOV) A.G.; KWPP, D.M.
Recurrence form of Seidel sums expressing the dependence of
aberrations on the position of the pupil of an aspherical
objective. Opt. i spektr. 18 nt.3:501-504 Mr 165.
(MIRA 18:5)

with Waimmou Spbolical
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u lot 14 .~Al ", .41all Al..I 11"
-11.1vatig file
A I.,. I ml liglol. WA. 11,40 its 1"I"

.1 INS h 14 370111
alculaum of th* lump of slopie woctrultalle
UAW. 4. 1.4.411 ( INU .1, 4d N. I R '. N
lo-viA %tu6 h irpoo u tit s) o. ec~ .I
1.1 1441W IMIA110 111lit-1-1 j-
;V., i'. ... all.. alml 10.6%11og
:Im. iwis 11"1f j.6411- oll 11'. Alt,
-t It,) #114U.41. .11 li,1.9.116-1 itill,
lh.'i ju, -311tkIllig wilb the 'fKAI All. A
jua'tu~l. j. I"U11.1 s,.&qI4yInx rquAll-a
.1ti Its low t.,Ulukd I'y the rhOll.1s, .1.1
gIV4-ts wdu,.. 41 W.
I. A...... 11-8 the ..a , Z,
In- 1.1.1 1... It-,, ".- "I
Vital filt.f. jilol.l. 11,
N., A-I I", l."X). It A.1, nott.1 ill I.Mj .'f jul.

VLA30V, A.
"Calculation df Fields of the Simplest zlectrostatis Lenses" and "A Short
Magnetic Lens with a 111inimum Spherica.1 Aberration," both abstracts of papers of
the Acad. Sci., USSR. Published in J. Phys., USM, 1945o Vol 9, No 1, p 60.
SO: ,dirless Engineer, iol 23, No Z74, Jul 46

?''B'WiTTV lilt ii
ju . t,0 a 41 4j $I id arte
AA It Q-A* JL'j s J,Ia j i t s a
o0 -40
00
oo lee
oe 81;- 3934. INFLUENCE Of NIXCTRODN PRZCIPITATION ON OPERATION Or
got ELECTRICAL PRECIPITATORS. V
ISmAso A. and Xapteov, N. nee
00 (J. Tokhn. Fit.* Nov. 1947, volo 17, 1371-1380). 200
00-3 Experimental investigittions have shown that a layer of 400
eo j non-conductinp particles on the electrode of a precipitator &;Of
distorts the field distribution ih the corona son*.
0e Measurements indicate that the outer corons. layer is charged
z to a certain potentials depending on the properties of the goo
=H' precipitate, thickness of the layer and corons, current. r.. 00
The tests wore corked out with reference to negative goo
corons,
discharge. Voo
'41 E.R.A.
goo
.1111, 0. .1.1 #11 lee
V IrsI t I 'W 0 i a I W 0q 48a 1rT

PHASE I BOOK D.PLOITATION SCFV/5035
Vaesayuznoye soveshchaniye po, stekloobraznomu sostoyaniyu. 3d, Leningrad, 1959-
Steklodbraznoye sostoyaniye; trudy Tretlyego vsesoyuznogo soveshchaniya Leningrad,
16-20 noyabrya 1959 (Vitreous State; Transactions of the Third All-Union Con-
fere ce on the Vitreous State, Held in Leningrad mNove*erl6-2O, 1959) Moscow,
Izd-vo AN SSSR, 1960- 534 P- Errata slip inserted- 3,200 copies printed.
(Series: Its: Trudy)
Sponsoring Agencies: Institut khimii silikatov Akademii nauk SSSR. Vsesoyuznoye
khimicheskoye obshchestvo imeal. D.I. Mendeleyeva and Gosudarstvennyy ordena
Lenina opticheskiy institut imeni S.I. Vavilova.
Editorial Board: A.I. Avguztinik,, V*P# Barzakovskly, X.Ao Bezborodov, O.K. Botvinkin,
V.V.Vargin, A.G. Vlasov, K.S. Yevatroplyev, A.A. Iabedev, M.A. Matveyev., V.S.
Molchanov, R.L. Myuller, Ye.A. Poray-Koshits, Chairman, N.A. Toropov, V.A.
Florinskaya,, A.K. Yakhkind; Ed. of Pablishing House: X.V. Suyorov; Tech. Ed.:
V.T. Bochaver.
PURPOSE: This book is intended for researchers In the science and technoloa of
glasses.
-22
Cav*

Vitreous State (Cont.) SOV/5035
COVERAGE: The book contains the reports and discussions of ihe Third All-Uaion
Conference on the Vitreous State, held in Leningrad on November 16-19, 1959-
They deal with the methods and results of studying the structure of glasses, the
relation between the structure and properties of glasses, the nature of the
chemical bond and glass structure, and the crystallochemistry of glass. FIMsed
silica, mechaniem of vitrification, optical properties and glass structure, and
the electrical properties of glasses are also discussed. A n=ber of the re-
ports deal with the dependence of glass properties on composition, the tinting of
glasses and radiation effects, and mechanical, technical, and chemical proper-
ties of glasses. Other papers treat glass semiconductors and soda borosilicate
glasses. The Conference was attended by more than 300 delegates from Soviet and
East German scientific organizations. Among the pexticiWts in the discussions
vere N.V. Solomin., Ye. V. Kuvshinskiy, Yu.A. Gastev, V.P. Pryanishnikov, Yu. Ya.
Crotlibi O.P. Mchedloy-Petrosyan, G.Po Mikhaylov, S.M. Petrov, AoN. Lazarev, D.I.
TAvin, A.V. Shatilav, N.T. Ploshchinskiy, A.Ya. Kuznetsov, Z.V. Degtyareva,. G.V.
Byurganovskaya, A.A. Kalenov, M.M. Skornyaov, P.Ya. Bokin, E.K. Keller, Ya.k.
Kuznetsov, V.P. Pozdnev, R.S. Shevelevich, Z.G. Pinaker, and O.S. Molchanova.
The final session of the Conference was addressed by Professor.I.I. Kitaygorodskiy,
Honored Scientist and Engineerffl Doctor of Technical Sciences, The following
Card 2/22

Vitreous State (Cont.)
90V/5035
institutes vere cited for their contribution to the development of glass science
and technology: Gosudarstvennyy opticheskiy institut (State Optical institute),
Institut khimii silikatov AN SSSR (Institute of Silicate Chemistry, AS USSR),
Fizicheskiy institut AN SSSR (Physics Institute AS USSR), Fiziko-tekhnicheskiy
institut AN SSSR (Physicotechnical Institute AS USSR)-, Ihstitut fiziki AN BSSR,
Kiink (Institute 'of Physics, Academy of Sdiences, Beloruss~aya SSR, Minsk),
Laboratory of Phy0ical. Chemiqtry of Silicates of the Institut obahchey i neorgani-
chesk6y khimii-AN BSISR, Minsk (Institute of General and Inorganic Chemistry,
Academy of Sciences Belorupskays SSR., Minsk), Institut vysok6molekuiyarvkh
soyedineniy AN SSSR(Inatitute of High Molecular Compounds, AS USSR), Gosudarstven-
nyy institut stekla (State Institute for Glass), Gosudarstvennyy iastitut stek- -
lovolokna (State Institute for Glass Fibers), Gosudarstvenn'yy institut elektrotekh-
nicheskogo stokla (State Institute for Elfectrical Glass), Sibirskiy fiziko-
technicheskii,ihstitut, Tomak (Siberiad Physicotechnical InstAtute, TomBk),Leningracl-
sk1y gosukustmmyy-universitet (rAningrad state university), Moskovskiy khimiko-
tekhnologichebkiy institut (Moscow Institute of Chemical Technology)jleningradskiy
tekhnologicheskiy institut im. Lensoveta (Leningrad Technological Institut imeni
Le~sovet),, Belorusskiy politekhaicheskiy institut Minsk (Belorussian Polytechnic
Institute,- Minsk), Novocherkasskiypo3-itekhnicheskiy institut (Novocherkasok
Polytechnic Institute), and Sverdlovskiy politekhn~cheskiy Institut (Sverdlovsk
Card 3/22

Vitreous State (Cont.)
SOV/5035
Polytechnic Institute). The Conference was sponsored by the Institute of Silicate
Chemistry AS U8SR'(Acting Director - A.S. Gotlib), the Vaesoyuznoye khimicheskoye
obshchestvo im. D.I. Mendeleyeva (All-Union Chemical Society imeni D.I.'
Mendeleyev), and the Gosudarotvennyy ordena Lenina opticheskiy institut imeni
S.I. Vavilova (State "Order or Lenin" Optical Institute imeni S.I. Vavilav).
The 15 resolutions of the Conference include recommendations to organize a
Center for the purpose of coordinating.the research on glass, to publish a nev
periodical'under the title "Fiziks i khimlya stekla" (Physics and Chemistry of
Class), and to join the International Committee on Glass. The Conference thank
A.A. Lebedev.9 Academician, Professor, and Chairman of the Organization of Com-
mittee; Ye.A. Poray-Koehits, Doctor of Physics and Mathematics, Member of the
Organizational Co=ittee; and R.L. Kyuller, Doctor of Chemical Sciences, Member
of the Organizational Committee. The editorial board thanks G.M. Bartenevi,
M.V. Vollkenshteyn, L.I. Demkina, D.P. Dobychin, S.K. Dubrovo, V.A. loffe,'and
B.T. Kolomiyeta. References acccmpwW individual reports.
Card 4/22

Vitreous State (Cont.) 9011/5035
TABLE OF CONTENTS:
Foreword 3
GENERAL PROBLEMS OF THE VITREOUS STATE
Basic Methods and Results of Studying the Structure of Glasses
Lebddev., A.A. (Academician., Professor]. Studying the Structure of Glasses by Means
of Spectral-Optical Methods 7
Poray-Koshits, Ye. A. (Doctor of Physics and Mathematics]. Diffraction Methods
for Studying Vitreous Substances 14
Vogel, W. (Schott Glass Works in Jena, German Democratic Republic], On the Cel-
10A Structure of Glass 24
Vlasov, A.G. Natural Oscillations of the Glass Lattice and Its Structure 30
Card 5/22

M
Vitreous State (Cont.) Sov'~035
Markin, Ye.P., V.V. Obuk-hov-Denisov, T.A. Sidorov, N.N. Sobolev, and V.P.
Cheremisinov. Vibration Spectra and Structure of Glass-Forming Oxides in
Crystalline and Vitreous States 207
Sidorov-1. T.A. Molecular Structure and Properties of Crystalline Quartz 213
Brekhavskikh., S.M... and V.P. Cheremisinov. Study of the Structure of Lead
Borate and Bismuth Borate Glasses With the Aid of Infrared Spectroscopy 219
,_j2,s.qvA.Q_. Quantitative Correlation of the Ordered and Disordered Phases
V I
in Glass 22-2
Bagdyklyants, G.O., and A.G. Alekseyev. Electron Diffraction Study of
Vitreous Silica and Lead Sil4cate Glasses 226
Kolyadin., A.I. Anomalous Scattering of Light in Glass 230
Card 10pop

Vitreous State (C.Ont.)
Discussion
Final Session of the Conference
SOVI'l-035
522
On the State and an the Further Tasks Connected With the Solution of Glass
Structure Problems (Resolution of the Third All-Union Conference'H31d
During November 16-21, 1959) 528
AVAILABLE: Library of Congress
JA/dwm/gmp
Card 22/22 6-29-61

15(2)
AVTRORI so" Ol'on SOT/?2-59.5-1/223
T11114 Glass Sciewo an too WHY Xsnlel.,vo, Congress
(Ranks 0 t*kl- Aft VITT Mand.loyelskon 0-Y.8d.)
PZMMCLLS Steklo 1 keranik.. 1959, Sr 5. pp 1-4 (USSR)
AMIACT. In the beginning a proclawatio. of the TeX KPSS to the
Personnel of the building mtorlal Industries for a qualitative
a" tuftntlt&ti~ I="&" of praductins, Is mu%loned. The
Congress took plax. in Moscow In the second beat of March of
the current yeax ad as devoted to the 125th anniversary of
the #"&t scholexle birthday. Outst&a4lng obealsta of the
Soviet Union and the People's D-ocracies attended theCongres..
The primipal preblem, of the dty.loymat of ch.xi.tr7
cars
Alsouss.d at th. plenary meting. and the mating. of the
IS Congress matlone. Przf..sor 1. 1. XItygorodakly opened
"a matines of the sub-moti.n for glass &ad gave a screwy of
the stages or devolopmat Of Soviet Class produotion as well as
Of a amber of proulsing task. In -he field of glass technology.
Moreover. the fall-Ing lectures dre held, Doctor Kornai
(I%Oplo*o Republic of Hungary) Investigated the

Card 1/4 structure of
vi
sa top-layers of class,

.j,AYJMNIlV.ik (ITS I. .. I L*nsov-t) discussed iis forsetla'aj
of a finely dtoperve; cr7stalliss phase frQ1% the 6144-like
phasel V. V. fargis and (;,-Q-K."pt7xA (COI) reported on I
ba
ti
t
hotochemical
r
u
l
a
l
l
ti

o
un
n
acence, s
orp
spec
re,
oper
as
p
p
:
f *.rim-Claw. typeal A- (001) r-Portqd a the
%matlutivo realproc. .
Istio.. between ordered ad dLa-
ert."4 glass p3n." T o~ _Apo ra
J-9s"s, Institut kht"i
Willkstav AN 533R (;LtItut* of Silicate Chexistry or the
AS USSR) d1scus-4 the reasons for the d1saarsemat on the
pr.bIsm of the tructar. of slasa-lik. sulstawass Professor
O.-&-lallinkin, 2. 1. Annalch, and M. Institut
tokla, (class luatitutoT -"parted on the Investigation of the
:;&.a Structure by the Kthod of Theresa Analyst- -A Optical
Pals,".Ationj To. V. P.4ushka (001) discussed the an. method
t *Iootrla el"s "I-T-tgaa the "Itiag of ailloatom by owns
high-rrequency currentl To. C. ShtoyaborC reported as
glass* jtjou-%-j-*ad ad bm. far r.Aow.
&M aajolloa which have twfu developed In the Ca"darstvoncLyy
R."haa-lo.lodom"I-skiy k.r--Ich..kly lastitut (Ste%.
3al.stifio Research I.AtItut. of Cor-doo)l L. S.
card 2/4 V
J~~h- - - (GOT) dla.usmd the role played y-W.
surface protection film In the destruction of silicate clas"al

_j�pbpre (001) discussed the colorlse baractrlstl. a
4. E.: IF
Glad thateah"A." of phosphate glaw".1 O-V-"A~gta (ITT)
reported a the -bl2,lty of **dim I." In glee. type. of
mysse. So. O-RO-310,1 Z. A. Rosa.. (III Stroykersaika)
Z
-
dl.aw.mj
abdudng the Close. by lead
the
azl" and alr~.siteal L.
"jj!Ajqh.uxa, Kher-ka,akly
_
leatitut (Vnertko~ Polytechnic Institute)

IWO& silicate r.rawtI.A ..A int.ring processes 19, the
80pov
.
br2qdPVftd Ila.. Layorl 1. V. TtrAlroo-Y I various
types of glass, 0,_!. jkoj~jv,701ad. Institute) roport64 *a the
det.r.inattoa of L.Faxlti.s LA .&Ila. b t I ly.log
y op" ",G:

4. S. N.Cdazav.. -a To. W, Orl.'a (Glass lastit"
T
ol.atro" gUse-Ishlih has be** d..Iood UY the..
. (GIaso Institute) discussed the kinatle. of
.r:r
S1 or erystallIzation center. in phato-sonsitive
of Cleo. j Z. N. Byrit.kay. (Glass lustiest.) di.eu ... 4
Us result. of the of the tendency of ph-phsAia
systeas toward. Ila&* forastloal "_A._qrechAAik.
3. T-211"'71Lh. &=4 a IM) "Part d oN 4110
&wvs:~&.tlsa of type* vf -.Lconlu~tlsg side Class a. In.
beal f V20 5 1 1. 1E. L. A. CEtch&aik, 1.
&M To. 1.-Psrp~rg (SIZES) disco ... d the production of
m-duatlV7. ril. an types of glans which contain oo-pacento
easily to be "Comrst.d.

Iyu,
P="=C&Lt Slokle I kocaalka. t960. ft 3. 43-46 (V331)
ANSELLMs The 3v4 All -Vat a Coot %W- On the Vltre~ U-14 vat halt it
Lexindr.4 at th: and .71959. It mo organis*4 bf the 1-11tri
kunil 012"Alat, Al 03SR (rantitato of the cb.ul.tr7 cc 2111-tsm
AS 9332). Todsoynsmys "ht-141*skoye obabob.sive I ... I D. r.
Mosdoleyv,& (All-Valon CheaLsal Satiety Intel D. 1.
" A a A&Z STSEV7 optlabookIz latatitat issal S. X
(844:102mal 1"Illoto is-at S. 1. T.Wilow). x4r.*41." Wa
reports on,the otruct." of in-stiglion uwtho3s of
vitreass a &t0. the "Ob"i" of vitrIfiestion &.4
&a4 %mbAI.Lx proportion at glasses *are 4.14-r*4. Th. C.21-.-~.'-.:4
9.4 opes.4 by AaA4*zLo1&x A. A. LOodow. Fazi".A1.1
"Shod. &M revalto oancezaixg the glass siratlars *or* Ali-... I
as %be lot meting. Acadwalclan A. A. Lobadev report*l an
ties "A revalto --f apticaL mthale, To. A. ror.y-t.ahtis 0. t"
dltrr"llon sethods 1. a. Tovatroplyov on general probleaj aj~:
Card rrafts struolvzo and Proportlas of classes. Th# 2ZI X.Su~j
reports on the prololoa of 1b. w,itre.uw . to '.oil L.
.CbA&I~Al PGOU112XIII&S J_
of 1~re=s
N. A. Corn-.
:On traprollom of C.afarialti.. of the VltrIflc.U1-..i s i. i--,
;Ies
Polyxor*1 A. 3. Zaawal-Ur, 'Theari, of Cl-.
A. 0. Vlajov, -Notaral 0.oMWfi~iaof the Class Latti.0 3rd
'i-IMU'PSAunss 9 reports On sawreallgallou r.#mlto of ojlla~~a
solid and so problato of the mobahlaa at witrifl-allont A.J.
.04 the of the Ursation of tha
se. . the X-le, 0. K. bot.jr-kla' -rro.-3. or
tifitAIGA %a th* Stotatux. of f-ttAl'ikh. T'.ift
"a TA-1-XL'-1'-Qlt-'. .0. the Stru.tore of iil-ti~j 1.
&ad 0. A. Tesin -Themaynaania properties at the Siliaa%e flr4tons
Poo - . - is.' 2
C~ &A4 C&O - A1203 - Sio -1 0. U. S&Zt.A.I. -U.ob"t-
not wA Strualral X. I b1. , -X'ohtzj'a
of Vitrifl-at W. At the 011 "sting, 13 wilb rrubltzv
I
of the $Ltae structure and optical Itvaatis.tiou s..ho!s1-Y "-I.
jM2xj-.sk*z-' -Wr".d Aofl.atl.. Spectra of aadlum Sillost clat'~'
sAd Their 2.14146S. %* %be Struct%r0i L.
do.kal4esso uspor2l.4 of Light "4 =0
;
I.Msos:~Jjv A_0-1~ltuXa. -3havostigstica of the YlUzativ..1 1;.at-.
of Alum si
T
I So Classes-$ 1. N. dabol- reported an Skis wart of
Card 2/ a lb. Ylalch.skjj ZW%ltnt AN S= (InallSele of Phyaiaa A3 t3L3) jib
classes free onj' souponint, -'with- to tropho to---
A 31 a:*, r.vorl.,% On
::try and the llmkal~lxaena; 61:7;ralanl T. t 4
a 001-slar stmature and Q roporlia. ; be orysAallluo q..rtvj
11. Drokh"'kikh and V. P. ch-l"Beialsov "Parloa .. .%-- ---I
in"otl,pti, 4: l..4- _. Elamite Ith the aid of
Infrared apsotreacopyl a. 9. Tlsotv. 'T-'. (t-X1t1%9%tw0 2-1-tt-% Of
the Orderly and 1rrwgOi&-rM`WwfA-Q1&vs-l Sad
A a A% k lavo*t1g~iian of it. kruat.ro
Vjfv'A. T.L. a Us to on
-4-0 ... -0. the 3trg.t~r. of a So I - r
Th.rool TrOsS240-1 1. 0.
Ajl4Z2j%y, V. 1. lrr2-nol. X. A. Voyah1110. 13tr-.t.r.l Takef-
W~totion Light In 5adjon- --1'
borom-ailleato at&&*.& . A% the Sth e.ting. 9 reports dealt, Ob I
tb. in".t tgn ,on "@.It* of .*41-baran-aillo-to 910-4-0. : A.
Appen and Can- ft-31. 'Boron and Al-ONO-M A-0-417 Of 1ht Pt'4P*r-
f Stlia:10 al-go To.31 colant, '00 %be C-.rdlawtva ;..-
Class..-) S. P. UdLu-v t.ported
f A2"I - and ro Is 0
on stroatural sheave In boron-ollicato glasseal To. A. povkr~xoablto
rtparl.4 can%roverstal probl... ..%tsr.lug
a
-atheir part..
Kowhits and 1. S. Ldr:yov, -3ubutGro*-QPlQ Uh--
In the St~ota,w of Coopl x 01 ....... Th. 15 r.,ort
card 3/8

TUSOV, A.G., dote.; MINKIV, I.M.. inzh.
Determining the electric field in a dielectric in con-
nection with high-frequency heating. Izv*v7s.u(:heb.zav.;
energ. 3 no-3:47-55 Mr 160. (MIRA 13:3)
1. Gosudaretvann" ordena, Lenina opticheakiy institut innni
B.I.Vavilova.
(Dielectrics) (Induction heatint-,)

VLASOV. A.G.; KRUPP, D.M,
Calculating the fields of electron lenses. IzvXX MSR.Ser.fiz. 2~
no,6s662-664 je 161. (MIRA 14:6)
(Electron optics)

396'1M
S/051/62/015/002/009/014
14. 3 -'0 E 0 3 2/ E 3 111
AUTHORS: Yermolayev, A.1-11. Minkov, I.'m. and Vlasov, A.G.
TITLE: A method of calculation of the optical properties of
a multilayer coatinS with a given reflecting power
PERIODICAL: 'Optiha i spelctroskopiya, V. 13, no. 2, 1962,
259 - 265
TEXT: The authors consider the design of an n-layer coatinZ
with a 'given reflecting power R. , where
R RN N+l, (1)
N
X. are the optical parameters of the media,
is the angle of incidence, and
X the wavelength.
it is required to determine the number of layers N' afid the
magnitude of the parameters x for which the reflecting pourer
Card 1/3

S/051/62/015/002/009/014
A method of .... E032/E314
a given an,-le
in the given wavelength interval and for
of incidence should be described by a Sivon function
RN(x 1, X?1 ... XNT* I X) = FOW (21)
The calculation starts with an assumed approximat -aly Icnoi-nn
function F 0(7,) , which is denoted by Rm and dontalins '
the arbitrary parameters x * The next approximation is
obtained by considering the quantities 6 , M.= M M + I.,
which are given by; M 01 a
k dX, It> '0 (3)
X) W 9 (X1 F (h)
m 0
In this formula W"> 0 is a weighting function,
Card 2/3 X is a vector whose oartagidn , coordinatAs irn