SCIENTIFIC ABSTRACT A. FREYDLIS - S.M. FREYDMAN

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• Collection: Scientific Abstracts
• Document Number (FOIA) /ESDN (CREST): CIA-RDP86-00513R000513710004-0
• Release Decision: RIF
• Original Classification: S
• Document Page Count: 100
• Document Creation Date: November 2, 2016
• Document Release Date: June 13, 2000
• Sequence Number: 4
• Publication Date: December 31, 1967
• Content Type: SCIENTIFIC ABSTRACT

FRe,TI)LIS, A.
Improvement in imings sharpness. Radio no.3:46 My 154. (XMA 7:5)
(Telovisim-Receivers and reception)

MYDLIS, A.
Automatic sound blook-system for radio reception and rodiffusion
centers. Radio no.10:42 0 '54. OWA 7:11)
(Radio-Transmitters and transmission)
1 1.
I
I
v

ussHl Zctradca
Card 1/1 Pub. 89 - 30/40
Authors I Froydlfso A.; Koteltnikov, N.; Pavlenko, V.; Tyushnikoirp E.; Trapeznikov..
1M1'!V1-V-L-W-UJ-, V.; Tkachenko, L.; and Nechay, V.
Title i Exchange of experiences
Periodical i Radio 10, 42-430,Oct 1954
Abstrart i Several small articlesp sent in by local radio operators,, are featured
under the above title. Each author offerso for the benefit of the others,
the results of his experience in the field. of electronics. The follawing
equipment and subjects are dealt with: an automatic safety device for the
protection of rural radio-center personnel agair-st electric shock; a min-
iature signal generator; an "interference-free" receiving antenna; a radio-
relay station of the Urozhay type; a Piezoelectric pickup for an electric
guitar, and others. Diagrams; drawings.
Institution: .....
Submitted:

VEKSM, V-I,; RRZNICHWO, M-S.;
Determining C-terminal groups of vegetable proteins by the thlo-
hydantoin method. hothisita 25 no.l:-124-128 Ja-F 16o.
(MIRA 1316)
1. Chair of Chemistry, Institute of Soviet Trade. Leningrad.
(PROTICINS chem. )
(HYDARTOINS chem.)

3119,90
83801
S/035/59,/()00/003/007/039
A601/00i
Translation from: Referativnyy zhurnal, Astronomiya i Geodeziya, 1959, No. 3,
P. 31, # 1903
AUTHORS: Dorman, L. I.. Freydman ! G 1.
TITLE- A Burst of Cosmic Ray Intensit February 23, 1915,15, and Its
Interpretation
PERIODICAL: Tr. Yakutskogo fil. AN SSSR, 1958, No. 2, pp. 129-1(39
.EXT- Experimental data on the burst of cosmic ray Intens:~ty which took
place on February 23, 1956, are systematized and studied 'Che data from 37
stations located in geomagnetic latitudes from 83 0 n.lat: to 73 0v.lat. were
processed. The distribution of the burst effect over the globe Ut different
instants from 3h5Om to OhOOM universal time was investigated. D, was discovered
that in the first period of the burst a sharp anisotropy was observed with an
Xdditional fliix of particles from the Sun; half-an-hour later, the flux of
solar particles'was "broadened" and approximated an isotropic one. The energy
spectrum of solar particles was found for Individual time instants. The resLIts
obtained were Interpreted and the possibility of generation of rolativietic
Card 1/3 --

83801
cz/035./59/000/003/007/039
AOOI/AOOI
A Burst of Cosmic Ray Intensity on February 23, 1956, and Its Interp'retation
particles on the Sun is discussed according to the following hypo*,.hesis-.
acceleration of particles on the Sun in the chromospheric flare 1:5 mainly brought
about by a statistic mechanism on account of the energy of magret.1c fields and
kinetic motions in the flare. Only in the first moment a mcre rapid accele-ration
mechanism should be in operation, similar to acceleration of particles in the
p.inoh-effect. The mea 102s,-c, the ra:ng-,
,~ life time of particles in a flare is
for scattering ;?, 2xlO cm, and disorderly, speed of magnetio f4 nld hcrterogeneit_' es
_~~3x,070m/sec. Going beyond the limits of a chromospherin, f~arc-, acselerati~d
particles diffuse in the "supernorona" of the Sun with th,~ ni-an life time of
,--103 sec and the mean scattering range of ;V1012C.M. lh~4 d4msnstons of the
carona then proved to be >,,, 7X~012cm. The particles abandon the "superecrona"
symmetrically to all sides. A fraction of the particles, moving along a straight
line, hit the Earth immediately after the ejection (anisot"ropic flux :in the
first period after the flare begir~ning), the rest of th-~ partle'les,eJected along
other directions than to the Earth, may hit the Earth only after scattering in
the interplanetary space by the magnetized clouds,, corpus,~ular fl-ax.~s with
frozen-in magnetic fields, or by other formations. The axth.ors disf,'ass t-ht~
Card

83801
S/035/59/OOC/003/007/039
AO01/AOOl
A Burst of Cosmic Ray Intensity on February 23, 1956, and Its Interpretation
problem of Injecting the particles and energy losses and sharg that relativistic
electrons should be absent in the fluxes of solar cosmic rays, There are 29
refp-rences.
L. 1. Dorman
Translator's note: This is the full translation of the original Russian
abstract.
Card 3/3

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210) S()V/56-36-3-65/71
AUTHORS: Gaponovo A. V.9
TITLE: On Electromagnetic Shock Waves in 7errites (Ob udarnykh
elektromagnitnykh volnakh v ferritakh)
PERIODICAL: Zhurnal eksperimentallnoy i teoreticheskoy fiziki, 1959,
Vol 36, Nr 3p pp 957 - 958 (USSR)
ABSTRACT: In the.preBent "Letter to the Editor" the authors investigate
the propagation of plane homogeneous electro.~agnetic waves
in a medip for the case in rhich induction t and field
strength 11 of the magnetic field are in nonlinear connection.
The medium is assumed to be isotropic and that B-B(H),
v(H) =W~H. Basing upon the Maxwell (tiaksvell)equation
and its partial solutions, the authors in the following
investigate the boundary conditions holding for the field
on both sides of the discontinuity, raid subject the front
of the electromagnetic shock wave to a thorough theoretical
investi,E.~ation extending, for the time being, to the simple
cane of a plane homogeneous wave in ferrite which is magneti-
ed up to saturation point by a homogeneous magnetic field
Card 1/3 i
, which is longitudinal with reopect to the direction
o

On Electromagnetic Shock Waves in Ferriten SOV156-36-3-65171
of propagation of the wave. For the connection of M
(magnetization) and IA (z,t) it holds that
4 1
W3t + Ho~_X M-IRrm, + H0]]
(y. magnetomechanical ratio for the electron spin,~ -1/,t0..
r6laxation frequency). Further, the case le0is subjected
to a short investigation. As it is found impossible to
write down a general solution of the Maxwell equation in
consideration of (3), the authors confine themselves to
dealing with the case of a steady plane shock wave. For this
case ~ is easy to integrate the equ.-ition. The~esult shows
that rotates round the direction of propagation of the
wave z (precision angle T) with the velocity cj.~ /p,
CO HIcos 9/sing- - (H 4nM cos Q)~(Q - th It between
11 y 0- e ang,
U and z, the primed quantities denote values at a great
distance from the wave front, i.e. at z -4 - aD ). Ex-
pressions are further given for the time width of the shock
wave front and the special cases of strong and weak shock
Card 2/3 waves are described in short. There are 4 Soviet references.

On Electromagnetic Shock Waves in Ferrites SOV/56-36-3-65/71
ASSOCIATION: Radiofizicheskiy institut Gorlkovskogo gosudarstvennogo
universiteta (Radiophysical Institut '? of Gor'kiy State
University)
SUBMITTED: December 18, 1958
Card 3/3

InYDKAU, 0. 1.; SHAM, 0. T.
=no
Some results of the cowerison of
hard components during September -
Ser. fiz. no-3:116-120 060.
(Cosmic rap)
the variations in t-A neutron and
0--tober 1957. Trud;r WAN SSSR.
(MM 13M)

69416
s/141/60/003/01/008/020
Xi4- '71? E032/E414
AUTHORS: Gaponov. A.V. and Freydman, G.I.
TITLE: On the Theory of Electromagnetic ahock Waye~in
Non-Linear Media
PERIODICAL: Izvestiya vysshikh uchebnykh zavedeniy, Radiofizika,
1960, Vol 3, Nr 1, PP 79-88 (USSR)
ABSTRACTz The propagation of electromagnetic waves in ferrites and
ferroelectrics is usually discussed in terms of the linear
approximation. The present paper gives a detailed
discussion of the propagation of plane uniform
electromagnetic waves in non-linear media, ie media in
which the magnetic induction B depends non-linearly
on H. The paper is divided into the following sections.
1. Simple waves in a non-linear isotropic uniform
medium. Production of discontinuities.
2. Conditions on the Discontinuity Surface.
3. Structure of the shock wave\front.
4. Effect of the finite conductivity of the medium.
The Maxwell equations are written down iij the form given
Card 1/5 by Eq (1) and (2)4 the relation between D and z is L~

691,16
s/141/60/003/01/0013/020
E032/E414
On the Theory of Electromagnetic Shock Waves in Non-Linear Media
assumed to be linear. Special solutions of the:3e
equations can then be shown to be given by Eq ('5)
where c is the velocity of light in vacuum,
it M = dB/dH and f ( f ) and f (I) are arb itrary
functions determined by the boundary conditions,
Eq (3) describes travelling waves such that each point
on the wave profile moves with a velocity which depends
on the magnetic field at that point. If the
permeability decreases with the magnetic field, then
those points on the profile at which the numeri,.-al
magnitude of the magnetic field is large will move with
a large velocity. ronsequently, whenever the magnetic
field increases (in its absolute magnitude) in a direction
opposite to the direction of propagation, the slope of
the front will increase until the continuity of the
field vector breaks down (Fig 1). If u is not a
monotonic function of H, the situation is much more
complicated. The boundary conditions on the moving
Card 2/5 shock wave-front are obtained by assuming that its

69L16
s/141/6O/OO3/0l/oo8/o2o
E032/E414
On the Theory of Electromagnetic Shock Waves in Non-Linear Mcdia
velocity changes slowly in the case of a pLane wave.
The boundary conditions are given by Eq (6) and i.6a).
It-is shown that if the discontinuity in the travelling
wave is a weak one, then the behaviour of the travelling
wave can be discussed in terms of the special solution
given by Eq (3) and the boundary conditions given by
Eq (6a). The problem is thus reduced to the determination
of the position of the discontinuity in a simple wave.
Weak shock waves can only exist for a limited time. In
order to discuss the structure of the front of an
electromagnetic shock wave, the relation between B
and H and D and E must be known. In the present
paper a simple case of a plane uniform wave propagated
in ferrite magnetized to saturation by longitudinal
uniform magnetic field is considered, If one neglects
Card 3/5 internal fields, then the connection between the Ll~

69h16
S/141/60/003/01/008y'020
E032/E4i4
On the Theory of Electromagnetic Shock Waves in Non-Linear Media
magnetization and the magnetic field strength is
given by Eq (14) (Ref 7). The structure of the
front of the electromagnetic shock wave, ie the
solution of Maxwell's equations subject to Eq (14),
cannot be carried out in a general form. However,
the present paper succeeds in deriving the corresponding
solutions for a stationary plane shock wave. It is
shown that the frequency of
field components in the region of the front of the
shock wave depends mainly on the magnitude of the
magnetic field in the wave. The length of the front
is reduced as the magnetic field increases,, The
character of the structure of the front of the shock
wave is determined only by the properties of the
medium. There are 4 figures and 12 references, 10 of
which are Soviet, 1 English and I French,
ASSOCIATION:Nauchno-issledovatellskiy radiofizicheskiy institut
Card 4/5 pri Gorlkovskom univeraltete ~Scientific Research

69416
S/141/60/003/01/008/020
E032/E414
On the Theory of Electromagnetic Shock Waves in Non-Linear Media
Radio-Physical Institute of the Gor'Riy University)
SUBMITTED; October 21, 1959
Card 5/5 V(

s/141/60/003/02/012/025
E192/E382
AUTHOR: Freydman, G.I.
TITLE: Electromagnetic Shock Waves in a Strip Waveguid Filled
With Ferrite
71
PERIODICAL: Izvestiya vysshikh uchebnykh zavedeniy, Radiofizika,
196o, Vol 3, Nr 2, pp 276 - 284 (USSR)
ABSTRACT; The propagation of certain types of electromagnetic
waves in a strip waveguide, which is filled with ferrite
magnetised to the point of saturation, is investigated.
In the case of slow channels~ when the magnetic field can
be regarded as being independent of the magnetisation,
it is possible to determine a whole class of partial
solutions which are in the form of unidimensional travelling
waves. The equation cf motion for the magneti5ettion is:
bm 2
- = - y [ MHJ - X M- [M E mij 1 (1.1)
at
where y is the absolute value of the magnetomechanical
ratio for the electron spin,
X is the relaxation frequency,
Cardl/7 M is the modulus of the magnetisation vector.

6/141/60/003/02/012/02')
Electromagnetic Shock Waves in a StrE'WAN8eg'uide Filled with
Ferrite
In the case of slow changes, the derivative of the
magnetisation M with respect to time is zero. From
Eq (1.1) it follows, therefore, that.
Emil = 0 ; H = M
(1.2)
For this case, the solution of the Maxwell equations is
in the form of Eqs (1-3), where c is the velocity of
light in free space, E is the permittivity of the
medium, f is the arbitrary function and 'H 0 is the
initial intensity of the magnetic field, which is directed
along the axis Z . The solution represented by Eqs (1-3)
satisfies the boundary conditions on any ideally-conducting
surface which is perpendicular to the axis y
Consequently, this is the solution not onlN for an
infinitely extensive space but also for a ferrite plate
which is bounded by ideally-conducting planes (Figure 1).
In the case of fast magnetisation changes, it is not
Card2/7 possiblt~, to (dive an ~.-xact solution of the problem.
I C

s/14l/60/003/02/012/025
tl?2/�~82
Electromagnetic Shock Waves in a S r p veguide Filled 'with
Ferrite
A stationary shock wave is now encountered. A. wave
whose field is independent of the transverse coordinate
and which satisfies the boundary conditions on the
ideally-conducting surfaces can be taken as the fundamental
approximation for theshock wave. The field iomponents
in this case satisfy Equations (2.1), where 13 = H + 4WH
0 0
this being the initial value of the z-component of the
magnetic induction. For this approximation, the equation
of motion of the magnetisation can be written as Eq (2.2).
The first approximation can be determined by solving the
system of linear equations containing partial. derivatives;
these are represented by Eqs (2.3) and (9.3a). Eq (2.2),
which gives the fundamental approximation, can be solved
approximately. If the relaxation frequency X is
comparatively low, it is possible to employ the method
of the s lowly-c hanging amplitudes for this purpose. By
introducing coefficients y I and K (defined on p 278),
Card3/,7 Eq (2.2) can be expressed as Eqs (3-1). The parameter K
~C~

s/141/60/003/02/012/025
&1~2/Ejfi
Electromagnetic Shock Waves in a Strip a egu e Filled with
Ferrite
can be determined from Eq (3.2), where -0. is the
angle of inclination of the magnetisation vector to
the axis z . The solution of Eqs (3.1) is in the form
of Eqs (3.4), where q is a certain constant. The
magnetisation vector undergoes periodic motion, whose
period is represented by Eq (3.6), where F is the
elliptical integral of the first kind. Since! Eqs (3-4)
represent the integral of Eq (2.2), it is possible to
derive Eqs (3-7). For the case of weak shock waves, it
is possible to neglect the second term in the righthand-
side portion of Eq (3-7). By solving Eqs (.'.,7) and 3-7a),
it is found that the amplitude of the M x component
of the magnetisation is given by Eq (3-8). Prom this it
is seen that the damping time of the oscillat-ions appearing
at the front of the shock wave is given by:
MAB 0 (3-9)
Card4/7 while the period of revolution of the inagnetisation

S/141/60/003/02/01.2/025
E~22/Ea8j,
Electromagnetic Shock Waves in a Strip veg 3. Filled with
Ferrite
vector is expressed by:
M If0
T Cl-' - -- (3-10)
yB0 H2x
The above analysis is not valid for the region where the
magnetisation vector only just begins to be deflected
from its initial position. This process can be
characterised by time interval To 1 durinS; which the
magnetisation vector completes one-half of the first
revolution. This time interval is expressed by Eq (3-11).
From the above results it is seen that the structure of the
front of the shock wave in a strip waveguide differs
considerably from the structure of the front of a shock
wave in an infinite space. The difference is observed
not only in the dependence of the field components on the
Card5/7 longitudinal coordinate and time but also in the ~ <

S/141/60/003/02/012/025
E141 EJ8
Electromagnetic Shock Waves in a Strip a4e uide Filled with
Ferrite
relationship between the characteristic time intervals
and the amplitude of the wave. This situation is
illustrated in Figure 3, where the 'dashed' curve
represents the dependence of the M x component on z in
a strip waveguide, while the 'solid' line represents the
same function for the case of infinite space. Eqs (2-3),
whichiepresent the first approximation, are linear non-
homogeneous equations with variable coefficients. An
exact solution of these equations is not possible.
However, it is possible to give an approximate estimate
of the magnitude of the field components if it is assumed
that: 1) the variable coefficients in Eli (2.3a) can be
neglected; 2) the method of the slowly-changing
amplitudes is valid; 3) only weak shock waves are
considered. The field components for the first approxi-
mation are therefore expressed by Eqs (4.2) (p 283).
From these equations it is seen that all the field components
of this approximation are proportional to a small parameter
Card6/7 awM/c Consequently, the principal approximation, in which
kc-l",

s/i4i/60/003/02/012/025
E1424EJ82
Electromagnetic Shock Waves in a Strip a e uide Filled with
Ferrite
the wave is described by Eqs (2.1) and (2.2) can be
considered as being valid. Secondly, if aw /C > hi I m i >> IM eo~ el~ and JA are
0 0
slowly.varying functions in comparison to the eikonal If
only a function of Vt-z, one obtains
3/7-

26h2l
S/056/0/041/m/oi6/021
Reflection of electromdgridtic waves ... B102/B214
let
v
Ova's
(5)
7
W 4 + 110t.
(6)
where ~to is an integration constant equal to the frequency at the
point and ~O is an arbitrary constant. If aV lhll> ... jmOj>jnj >.
Then i f - 6,1
+t, one obtains approximately:
-..Card 4/7

2W1
S/056/6.i/041/001/016/021
Reflection of electromagnetic waves B102/B~14
(14)
V'; P'Pt. vt -(I
to
C (t WB VI. 1.2
The ratio of reflected to total energy is equal to
4
F I V ( I
I vo
*1;2 %0
and is larger than 1. -In the following the reflections of plane electro-.!,
magnetic waves i'n an unboy1ded plasma by the,waves of amagnetic field,
u'
by a niformly moving inhomogeneous plasma, and'by the ionization wavAs
of a plasma at rest, are analogously investigated. Reflection by the
(nonrelativistic) moying plasma is given by
It: Ij = F- -
(Vto' T 0 hpio'V
(20),
P*10 V -41OWUN.
CO-PI)
which is compared with (14). The amplitudes of the'inciient waves and
that'of the waves reflected by the magnetic waves obey'the law;
Card 5/7

-26WI
S105 61/041/()01/01(J/Q21
Reflection 6f 'electromagnetic waves ... B1 02YV214
x
C
x [Vr. "I + P (Vi. 6 + (01'pfixts (DH*),) x
C
x exp ~P do)m X (21)
C
dt
~x + -E dt
G)'N +
C (Vt -0)H? )I] .
The amplitudes on refleotion-by a moving plasma (a) and by- ionization'
waves (b) are:
4.1.2 el'.8 (4%, -(1 -PI) CO. (-.001/1v11. R-M WILWIPIP W;
(a) elle, - V1, Vt; 1.1 W/Ift; 1.2 (2 2
(6) , e,le, = 1. (p = 1.
In all cases considered the frequency, amplitude, and total energy of.the~
wave packet increase on reflection. The author 'thankb A.V. Gaiponov ford's
advice and discussions. There are 2 figures and-11 Yeferencee: 10'
Soviet-bloc and 1 non-Soviet-bloo.
Card .6/7

264 X
/041/001/Cil6/021
Reflection of electromagnetic waves B102 B214
ASSOCIAION: -Radiofizi'oheskiy instituf Gor1kovskogo gosudarstvennogo
univerBiteta, (Institute of Radio Physics of Gor1kiy .43tate
University)
SUBMITTED: February,69 1961
Card.. 7/7.
--- ---

S/056/62/043/003/053/063
'C' B100102
!!")Rs: Daur,,3, Z. Ya., Freydman, G. 1.
T
----------
TITLE: Dopplev effect in the reflection of an electrom,i6netic wave
from a mabnetization wave in a ferrite
4'k
P~-'. UODIC L- Zhurnal L-kaperimentallnoy i teoreticheskoy fiziXi, 1P
no. 3(9), 1962, 1102-1104
T1-2XT- The reflection of electromagnetic waves from magnetizinE waves -e'as
studied.in a coaxial cable'filled with AM-1 (AVI-1) ferrite ( 1
Su9ceptibility of the ferrite was varied spatially and .,.ith time
f ('z-V ~
00) by means of spiral conductors wound on -the coaxial cable.
9 1
The'velocity v 0 oil the magneti zation waves was 10 CM/sec' the frequency
of the incident ivaves ,,as 3200 Mcps, the frequency maximum of the reflected
vi.,.ves vi-q at about 3400 b1cps. The coefficient of pcwer refl,.~ction was
about 10-4. When the intensity of the constant maenetic field alonC the
coaxia-l'cable is 25-40 oe, electromagnetic waves are not reflected if the
' i
Gard 1/2)

S/0 '6 2/0 4 3A)03 /0 5 3/0 6,
Doppler -.~:fect --n the reflection ofs*4 B104 B102
'00 ov. There ~)re
f1fold otron-th of th.0 maenetization waves is less than
3 fiCures.
ASSOCIATION': Rikdiofizichosk!3~ institut Gor'kovsko6o
universitata (Radioph~sical Institute of the G01"..(j.y State
University)
SUBWITTP: June 2, 1962
F, i~. 1 . Section across the
coaxial cable.
LeCend:' (1) Coaxial
cable, (2) ferrite,
dielectric, (4) spiral,,
dielectric, (6) metal
3neath.
Card 2/2

L :LO12L-6a ~BDS
ACC9SSION BR: AP300010 s/oi4i/63/O()6/oo2/o324/0337
AUTHOR: ?reydiranj 00 IN
TITLE: shock waves in a transmission line with a thin ferrite coating -- I
SOURCE: Izvestiya vysohikh uchebrWkh zavedeniy.. radiofizika, v. 6. no. 2, 1963-t
3P-4-337
TOPIC TAGS: ferrite-coated transmission line, shock wave
ABSTRACT: The possibility is considered for studying the field of an electro-
magnetic shock wave propagating over a two-conductor ferrite-contalning line by
means of ordinary differential equations. By using a simple example of a
perfect-conductance-wall vaveguide, It Is pointed out that tke problem can be
reduced to an analysis of telegraph-type equations coupled v1j.th nonlinear finite-
order differential equations only for these cases: (a) a =a:-1 cross-section of
the line and quasistatic nonlinear relations between the mmg~ietic field strength
and the magnetization intensity and (b) a nonquasistatic magmtization and the
simplest line cross-section configuration. For ferrite-coat!d transmission lines$
Card 1/2

L 10127-63
ACCESSION M, AP3000156
ordinary linear differential equations are developed; they are derived from the
Maxwell eciuations and, jointly vith a nonlinear equation for wMetization
intensity., can approximately describe the shock-vave structure. Orig. art. has:
25 equations.
ASSOCIATION: Nauchno-issledomtellskiy radiofizicheskiy institut pri Gor1kovskom
universitete (Scientific-Research RadioplWsics Institute, G03"kiy University)
SUBMITTED: 13Jun62 DATE ACQ: 12Jun63 ENCL: 00
SUB CODE: CO m REF sov. oo6 OTHER: 00:2
/2
6rd

FREY" G. I.
I I
Shook wav" in trangniesion lines w1th a thin layer of ferrite.
Part 1. Izv. vys. udheb. zav.; radiofiz. 6 no.21324-.337 163.
(MIRA 16:6)
1. Nauchno-issledovatellakiy radiofizicheskiy institut pri
GorIkovskom universitete.
Radio lines)
lectramagnetic waves)
R

L 10277 F.PA(b)/ZFR/BW/WW-A?FTG/
ASD-Fd-!4/To 4-WW
ACCESSION NR: AP3000157 S/0141/6-3/006/002/0338/0347
AMHOR: FrVdman, G. 1.
T17LE: Shock vaveslin a transmission line with a thin felTite coating -- 2
souRCE: Izvestiya vysehikh uchebrWkh zavedeniy., radiofiz-!.ka, v. 6, no. 2, 1963,
338-347
TOPIC TAGS: ferrite-coated. transmission line, shock wave
ABSTRACT; It is pointed out that the necessary condition for the uniqueness of
the shock-wave leading edge coincides with the condition of its stabiliV in the
quasistatic approximation. The nonstatic field around the shock wave propagating
in a coaxial line, can materially affect (with sufficiently lr-rge cross-section
of the line) the parameters that determine the shock-w-ve stnicture. Mrgever.'
with strong shock waves., these pexameters differ but little from those determined
for the static approximation even In the cases when the leading edge width in
shorter than the separation between the line wa.11s. Dispersion of the douinant
mode in delay systems has a different influence upon the shock-vave structure.
Card 1/2
- - - - - - - - - - - - -

L 10277-63
ACCESSION NR: AP3000157
With the increasing wave amplitude, the leading-edge durat;ion in a comb-type
delay system approaches a finite value vhich depends on Vie dispersion
characteristics of the line. In addition., the dispersion re:3ults in oscillations
which follow the shock wave; the amplitude and period of these oscillations grow
with the amplitude of the shock wave. "In conclusion, I wn using this o;portunity
to express qr gratitude to A. V. for his attention to this work and his
valuable advices." OrJg. art. has: 19 equations and 2 figures.
ASSOCIATION: Nauchno-Issledovatellskiy radiofizicheskiy Lnstitut pri Gorlkovskm
universitete (Scientific-Research Radiopbarsics Institute.. Gor1kiY University)
SUBMMTM: 13Jun62 DATE ACQ: 12Jun63 ENCL: 00
So CODE: CO NR BEF SOV; 007 arm: 000
Card 2/2

BELYANTZFV, ~014,; FREYDMAII, G.I.
, , , "
I]Jeotmriagnetic waves of fin&l ampliude in coupled transuission
lities with nuO.inear parameters. Izv. vy5. ucheb. zav.; radiofiz.
7 no.3i514-523 164. (41W, 17tll)
1. Naucl~mc-issledovatellsldy radiofizlc~eskiy inatitut pri Gorlkovskom
universitate.

(b)/DiT(1)/BDS/EP-C-12/0-EC(b)..~2-:..AFI~M/ASD/M-3
PA
Pd';
Ej~ ~h '~/0141163j'06/003/0536/0550
AC ESS ON NR* AP 004840
"5V
AUTHOR: F r eydman, 0.1.
TITLE: Effect of the linearli-approxi mated dispersion characteristic upop the
structure of shock electromagnetic waves In a two-wirf) transmission linere
SOURCE; IVUZ. RadlofizikA, v. 6, no. 3, 1963, 536-550
TOPIC TAGS: dispersion. transmispion line', shock wave, electromagnetic wave
ABSTRACT: If shock-wave processes occur so rapidly that they cannot be
described by the static nonlinear relation M v M(H) or P a P(E) , M being the
intensity of magnetization, P - polarization, H and E - magnetic and electric
field strengths; and if the field permeating the nonline-ax medium is essentially
Inonhomogeneous, the shock-wave structure cannot be! described by ordinary
derivatives. However. the article clarifies some po;~ knts regarding the shock-.
wave-front duration and the changes in the electromagnetic field before and
1 Card 1/2

L-15615-61
FACCESSION NR., AP3004840
Ibeyond the wave. It Is pointed out that the shock va! Whose front duration Is
shorter than a certain value determined from the linearly-approximated diaper-
sion characteristic of the system is absolutely unstable with respect to the waves
whose phase velocity is close to that of the shock wave. Aa the condition of
shock-wave stability with respect to low-frequency wayms is supposed to be
binding, the above value (except for some specific canem) roughly determines the
shock-wave front duration and some pacultarities of Its structure. Fundamental
itypes of dispersion characteiris tics and the corresponding front structures are
investigated. The front structure in also investigateii for a specific case of a,
coaxial -helical waveguide titinly coated with saturated forrite; the waveguide dia-
persion characteristics are analyzed. "In conclusion, I am using this opportunit
to thank A.. V. GancLnov for his attention to the work and. a useful discussion of he
t yl
11 Orig, art. has: 3 figures and 30 formulaiF-"
results.
1 ASSOCIATION: Nauc~no;,-Issledovatellskiy radiofizicheckiy institut pri
Gor1kovskorn univerpitete (Scientific-Research Radiophysics Institute. Gorlkiy
i, Univ rsitV1
19 Jul 62.
:1 ", DATE AN: ' 27 Aug 611 ENCL: 00
-1 slit CQP&Z_-;G0V PH NO REF SOV: 010 OTM 001

57-
't '55103-65 -04
_9WA(k,)/F8w/_#W6-K MAWPOTI&Ii Atc( EEC"t 4
h, ~_Prrr-41Pir-4j _SCP/1jP(0-Y-
ESC(b)-2/F_WP(k) (' ) /Po,~4/Pf -4/Pe~/Pll ept-4
014
ACMION HR t WGIW
'AUTHORt FreVAMAns (to i 1.
TMXt Effect of fine spli"IM of thi lover 1g"1 of Cr3+ In r*y an s=e char;
wberistice of coherelst wdssj~d
[SOURCEt IM. RaC110f1Z1JMS'V. 8. nos-2 1965 2*-284
ruby laser,, co oreut gelonj level--gplItting
TOPIC TAN:
ABSTRWTz TO determine the cause of the frequency. deviation o.! a r0y laser (red
shift) the authors derives _4~lified-equatione -describing .-theet3herent emission of
the-excited chromiva ions in v. ruby placed in a traveling-veve i= Aii
of the transient-response of.the laxersbased on a solution of these equations,
shows that the fine splitting, of -the lower level of the chraabin ion in the cryx-
a
tolline field of the ruby produces a change in the average freiluency of radiatio
-during the time of the transientsp ia a direction oppocite to 1hat produced by the
change in temperature (violet,shift)o -It Is shown that the larel lifetimes and them
dipole moments are highly sensitive to the. q of, the cavity in Aiah the ruby is
Cdrd 2/2

L 1571N65 94T(1)/FM-4/EEC(t)/EW(b)-2/WA(h) Feb ASD-31E0-31RADC1AXC/SSD/
Esp(MM (c)AtDc(a)/BSD/SSD(b)/P&W- iS.D(a)-~/ASD(f)-2/ASD(P)-3J~FM'R/RA&,(a)
ACCESSION NR! AP5000317 S/0056/64/0474"0135/1699117LO
AUTHOR:- -Belyantsev.- 44,
Gaponov, At. Ves, Daume, E Ira.; Freydman,
Ht
G, 11
TITLE: Experimental investigation of propagation of Unite amplitude
a
:_,lectromaj%netic wavesAn farrite-filled waveguides
SOURCE: -Zhurnal eksper mental,'noy-I teoratichaskoy J124ki, _v. 47, not
;5t 1964g 1699-1710
.TOPIC T-AGSt waveguide-,- waveguidewave propagation, fet:rite filled
------ wave
guiAe-#-- elect romagt~e-t1c.--shockvw evet-
A'BST1-(A-Vr -,of a
hoc -_waves--,-: a--av coaxial farrite-fill d*'
'wave P of T6d&--:'q `464 49, 1 4
Ote&:1 a t
cm-: Ong was inv6stigg
A high-re'-s-istance- voltage- divider, connected to the junction- of the
-voltage to a high-speed oacillo-,,.
.sections furnIshed the*_,controllLng
fi~ 4--of -tkesystem-permitte -muasurements
.Crap --of-wave-_
rite pass an
~front durations of Vasec and more.--The sections of.the,waveguLde
were. contained in-two solenoids with -a longitudinal field component
:up to 300 oat .The azimuthal component was formed by current flowing
:;Card 1/4

L 15710- 65
ACCESSIOWONR*, AP5000317
in- the Inner conductor- of the coaxial-wavegulde. Tubes _D_f P-1000
,ferrite'(Vith adielectric constant between 16 and 20) with inner and
'outer diameters of 8 and 16 mm'enclosed the inner con4uctor. The
formation and-propagation of-stock-waves were investigated Uret-with
:two patterns of permanent ferritemagnetization; longitudinal field
only and a field having both-longitudinal and azimuthal components,
Then- -the-samG-Investitation-was-carr Led out-with-nonnagmetized fer-
~,rite. Furthermore the structure of shock wave fronts was studied
under various conditions of ferrite magnetization. In t:he case.of a
ilongitudinal field the shock waves were found to result from-the
evolution of simple waves, Thus,.the input pulse would tend toward
increasing the,rise rate at its 'front, and flatten the trailing edge
so it propagates within the wave'SuLde , until (after a tk-de lapse _of.
about 200 nsec)~ a shock wave ensues. 'L. The amplitude d'epe,; dence of. the i~
of the shock wave -was meas.d,red -an&-plott.ed -f or dif f arant--
a-
longitudinal components 'of the' constant. field, In- the disie of
fien'tly qsg att ad ferrL filling having the .arlmut'hal- field
-perma a z te
compa'aan t~ dambinied with-the:'lon'ttudinal, disruptions diiveloped
u -as
Inder!certatu coxkdttion4i, front, as. WO at the''t aEl1nj4dj*,

T, 15710-65
SACCESSION NR: -AP500031
7
and within a certain t L me' interval, after which the jumps began to
diminish. The -phenomenon, however, was not ascribed-to evolution olf
a simple wave; the discontinuities appeared at the very entrance to~
the waveguide -it.-certaLn' values -of the current In the- -axial. conduct.or--1--
_;of the waveguide due to an Arreversible change of magnetization caused
;by increasing amplitudes o*f spin-waves. The experiments with'non-
magnetized ferrilte.confirmed the earlier results.obtained by Ostrov-,!
~skiy (Zhurnat teknichook,oy fittki, V, 330 19630 1050) who assumed.
that changes in the mean aziMuth*1 magnetization are caused by not%-
coherent rotation, After a certain time interval, a steepening of
~.the wave front sets in, due to dissipation. The ensuing shock wave
is structurally similar to a stationary shock wave, The shock wave
'front structure in discussed st.length under various experimental
conditions and withraference to earlier works on the problems orl&**~
art. has: 9 figures.
-,ASSOCIATION:, Ridi0fizicheskil institut Gor*kovslcogo gostidarstvennogo
universiteta -(Institute of R&diophysics,-Gor-~kiy State UmiveraltZ
Card

In
n--mc!
7~w, rpd r-,f.: Z
n r

L Q148-65 E-WT(1)/gWP(M)/E"(d)/EPR/FM(k 4A (h)/EWA (c) Pd-1#1,4 WW_
jACCM81OH HR-.- AP6010806 UR/0057/65/035,MW06?
7/0689
AUMOR: Bel ntsev, A.Mo; ov A.V. Fte
_ydman,0.1.,
TITLE: On the structu".of.electro metic~ shook fronts. In-nonlinea!r--transmiss ton, -
-lines
;SOURCE: Zhurnal tokhnicheskoy'fizIkI',_ v, 35, no. 4, 1965, 677-689
TOPIC TAGS- shock.wave, shockifront,structure, electromagnetic, wave" nonlineazity,
transmission line
ABSTRACT: Stationary solutionsof the,tolographic -equation with non1Jnear__:-.
-param-eters nre discussed -in terms. --The -system,is specified I~Iiy a pair of-
nonlinear functionals-giv the-- linear densities of charge and flux in ter-tas of
the current andL potential. Most attention Is given to stationary shi:,ck waves, i.e., -
to disturbances- that propagate -at -oonstant velocity with uncharWd Vxm but with
-dilferent'asymptotic values'of tho current far in front and far behiijd. Conditions
are derived,for the existence, of shook waves In two-conductor transm:19slon lines.
,Several simple specific cases, representative o9 general types of transmission line,
Card 1/2

-(i)/~WP(M)/EWA(d)/EPH/FCS(ir,)/EWA(h)/EVIA(c)
..ACCESSION,NR: APSOIOS07 UR/0057/66/035/004/069-0/0T04
Freydman 1. 1
AUTHOR: Belyantsev,A~M.;,Gaon A ___L(
TITM. On the structure of -shock waves In nonlinear t::ansmIssIon liras with
delayed.4xcitation of Internal degrees of freedom
.SOURCB: Zhurnal tekhnicheskoy~fiziki, vol.35, no. 4, 1965, 690-704
TOPIC TAGS: sh6ck. wave., shock front structure, electromagnetic wave, transmiss-
ion line, nonlihoarity, nonlinear differential equation
ABSTRACT.- This paper isa sequal to the preceding paper (ZhTFj 34, 1577, 1965,
/see abstract AP50108067 n which the authors discussed solutions of the tole-
graphiu equation with nonlinear-parameters, In the present paper the authors dis-~
cuss transmtssion lines for which~the nonlinear f6zationals giving the charge-and
flux densities In flux dew ities in termg.of the current and potent Jal Involve
two very different time constants, Methods are developed for the alipt-oximate
i separate treatment of the slow and fast processes. It is shown that the
approximato aquations containing. only the slow processes have d1scontLnuous solu-
tions correspondirg to shock waves ~wbon and oul when the phase spkne contains
Card 1/2

L49247~65
ACCESSION NR: APSOIOS07
singular surfaces of acertain type., -The important features of the dtsContinuous
solutions cau be determined from these singular surfaces, and the structure of the
continuous shock wave can be subsequently calculated by Including the fast
processes, -- -SeVeral-spec.tal cases . are discussed In considerable de,tall. An,
ascillo it
gram is presented of the shock -front-- in -a transadasion no Irwclving a
sat ating ferrite Lvductance and two RC shunt circuits with I
constants; this oscillogran Illustrates 'features of the calculated, shmk front
structure.- Orig. art. has: formulas and 12 figures.
ASSOCIATIOM. Nauchno-Ladledovatellskiy radiofizlcheskty institut pr:L Gor1kovskan
universitete Im. H.I.Lobachavskogo ~Badi2phr_!S~ Scientific Research platitutep
Gor*kI
-Y -Univerelt&
SUBMTMD: 03Jan64 EML: 00 -SUB WDR: EK
NR REF SOV: -,-OMM: 002
Card 12ja

T nAA1A_.A7 FWT(1)/FFr(k-)_9/T/EWP(k1 11P(r) WG
ACC Nit, AP6033285 SOURCE CODE: UR/0141/66/0091005/0919/0922
AUTHOR: Sushchik, M. M.; Fr ey dman. G. 1.
'ORG: Scientific-Research Radiophysics Institute at Gor'kiy Uni ersi y uchno-
V t - (Na
issledovatel'skiy radiofizicheskiy institut pri Gor'kovskom universitete)
TITLE: The width of angular and frequency spectra of radiation from a lager with a
nonlinear absorber i6'
ISOURCE: IVUZ. Radiofizika, v. 9, no. 5, 1966, 919-922
TOPIC TAGS: nonlinear optics, laser output, Q switching, nonlinear switch , laser
radiation spectrum, Q factor, laser emission
ABSTRACT: Field build-up time of a laser with a nonlinear absorber as a (1-switch is
a function of the spontaneous emission over a certain finite interval. Unless thus
considered, errors are introduced in the determination of the width of the angular
and frequency spectra of a laser and the dependence of these on, say, pumping energy.
Q-factor, etc., as was the case elsewhere (W. R. Sooy, Appl. Phys. Lett., 7, 37, 1965).
The problem is limited to a case of homogeneously pumped two-level molecules of the
active medium and nonlinear filter. Conditions for excitation of one type of cavity
mode are derived for &.laser with a nonlinear absorber and plane-mirror cavity. The
assumption that in the course of a giant pulse, differences in populations of an
active medium and nonlinear filter are independent of coordinates, in shown to be in-
valid. The results are valid only for T at T3 (where T - +T 1- 1, T, being the effective

nAA I A-A7

ACC NR. AP6022077 /_6 f 0 (- 0
k of4l_ 6- 0- 1- 0~ 3 3/0524
1AUTHOR. Bcapalov, V. I.; Freydman, G. 1.
-------------
:ORG: Scientific -Re search Institute of Radiophysics, Gor'kiy University (Nauc o-
hn
!Isslcdovatel'skiy radiofizicheakiy institut pri Gorlkovskom universitcte)
ITITLE: Spectral and energy characteristics of giant-pulses-
!SOURC'E: IVUz. Radiofizika, v. 9, no. 3, 1966, 513-524
TOPIC TAGS: giant pulse, laser pulse, laser R and D 1~
241
ABSTRACT: Although an examination of laser multimode processes describable by
nonlinear equations in the general case is extremely difficult, the spectral character-i
istics of giant pulses and pulse delay time (from the moment of completion of self-
excitation conditions) can be calculated with sufficient accuracy in a linear approxi-
mation. The development of the giant pulse, when the nonlinearity is esuential, can
be approximately described by equations reminiscent of those of a single-mode la,;cr,'
which permits evalwiting the effect of multimode structure on the energy and pooer of
the giant pulse. It is found that the irequency spectrum of the pulse emitted as a
Card 1/2 UDC: 6Z1.378.3Z5

ACC NR1 AP60ZZO?7
result of Q-switching is much wider than the spectrum of a single pulse -emitted underj'
ordinary conditions, The maximum width of the angular and frequency spectra and
minimurn delay time correspond to an instantaneous Q-owitching. A theoretical plot
of a W vs. no is in good agreement with experimental points obtained from a
Nd-glass laser (lZ-cm long, I-cm diameter rod). A typical numerical example
shows that two lasers - ruby and Nd-glass - have about the same parameters: pulaq
delay time, 24 nuec; angular spectrum, 5'. relative width of frequency spectrum,
0. 3. The effect of the number of modes on the giant-pulse height was determined on
a digital computer; a difference of only 1019 was detected between the multimode and
single-mode cases. Orig. art. has:1 6 figures and 37 formulas.
!
;UB CODI;: ZO / SUBM DATE: 3lAug65 / ORIG REF: 006 OTH REF: 003
Card Z/2

ACC NR, 'A P6022081----- - ______S_'0__UR_C_ '/05
CODE: UR/0141/66/009/0(13/0550 60
~AVTHOR: Frcydman, G. N.
10441, Scientific-Re search Institute of Radiophysics, Gor'kiy University (Nauchno-
proledovatel'skiy radiofizicheskiy institut pri Gor'kovskorn universitete)
LE: Frequency doubling in convergent partially'-- t;6herent light beam a
MCF,-.~ XVUZ. Radiofizika, v. 9, no. 3, 1966, 5.5-0-560
TOVTC, TAGS: frequency doubling,. coherent light
'BSTRACT: The geometrical -optics approx:imation used by D. A. Kleinman (Phys.--
AeW..,- 128, 1761, 1964 in analyzing the process of light-beam frequency doubling doefi I
otpwrmit valuating the accuracy of results and is inadequate for examination of the
requency conversion in the lens focus. Hence, the approximation of specified fix.fit-
harmonic field is used for obtaining exact integral formulas (sirw1ar to those
deve loped by D. U. McMahon at al. , J. Appl. Phys., 6, 14, 1965). By evaluating
he! integrals with a certain-accuracy, simple formulas are derived for the conversionl
actor, directional pattern, and frequency spectrum of the secondary radiation. It is 1
1 Z UDC: 6Z1.378.001

NR- AP6022081
round that: (1) The effect of finite angular divergence of the primary beam on the
ronversion factor is practically independent of whether the divergence is due to
partial beam noncoherence or to spherical waveshape of a coherent beam; (2) By
selecting an optimal focus length of the lens used for focusing a coherent beam
~spherical waves), the conversion factor can be raised by a few orders of magnitude;
~n focusing a partially coherent beam, the conversion factor may even fall off;
:3) Under practical conditions, the finite width of the primary-beam frequency
spectrum often has a substantial effect on the conversion factor. "In conclusion, the
iuthor wishes to thank V. I. Bespalov, A. V. Gaponov, and V. I. raAanov for useful
fiscussions. Orig. art. has: I figure and 50 formulas.
SUB CODE: 209
0 /SUBM DATE: 06Aug65 / ORIG REF: 007 / OTH REF: 003

FREYM-41i, I.; RATANOVA, V.; BILYXH, Ye.; SOSFIDOV. N.
Using methyl bromide for disinfecting cereal products and grain
in storage. Muk.-eley.prom. 26 no.7:12-14 Jl 160.
(MIRA 13:8)
1. Voesoyuznyy nauchno-issledovatellskiy institut zerna
produktov yego pererabotki.
(Methane) (Grain--Storage)

AUTHOR i sovA4o -58-3-29/34
TITLEt On the Theory of the Radical of an Associativi Ring (K teorii
radikala assotsiativnogo kolltsa)
PERIODICALt Izvestiya vysshikh uchebnykh zavedeniy. Matematika, 1958,
Nr 3, PP 225-232 (U=)
ABSTRACTs The present paper deals with a general theory of radicals of
associative rings. The main result is the following fact obvious-
ly suggested by Plotkint In an associative ring K let the S-
radical R(K) be defined in the sense of Kurosh [Ref 1_1 , whereby
some additional demandsere seumed to be satisfied. Then in K
there exists a ra( (K) ~aleo in the sense of Kurosh] con-
taining all bilateral 5-ideals and all commutative ideals of K,
while the factor ring K/ff(K) contains neither S-ideale nor
commutative ideals different from zero.
The paper consists of four paragraphs and contains 20 defini-
tions, lemmatal theorems and conclusions.
There are 9 referencesq 4 of which are Soviet, and 5 American.
ASSOCIATIONsUrallskiy gosudarst"vennyy universitat imeni A.M.Gorlkogo
(Ural State University imeni A .X.Gorlkiy)
Card 1/2

On the Theory of the Radical of an Associative Ring SOY/.140-58-3-29/34
SUBMITTEDs October 14P 1957
Card 2/2

AUTHOR: P A_(Sverdlovsk) _':0V/42- 13-3- 22141
TITLE: On the Theory of the Radical of an Associative Rir:6 (K teorii
radikala assotsiativnogo kolltsa)
PERIOEICAL: Uspekhi matematicheskikh nauk, 1958, Vol 13, Nr 3, pp 234-235 (USSR)
ABSTRACT: In the associative ring K let be defined a certain s-radical
R(K) in the sense of Kurosh, where the property s has to
satisfy the following additional conditions:
a) let every two-sided ideal of the a-ring be an a-ring;
b~ every ring, the square of which equals zero is an s-ring;
c let a be a local property.
The series
0 - A C A1CA 2 C ... C AC A +1 C.-*A ra K,
where the subrings AO(are two-sided ideals in A CK +1 and A DW /A oc
is either s-radical or commutative, is called an a-solvable series.
Theoremi If K has an s-solvable series, then its commutator K'
is s-radical.
Theorem: If K has an increasing series of ideals with commutative
Card 1/2 factors, then the commutator of K has an increasing series of

On.the Theory of the Radical of an Associative Ring SOV/42-13-3-22/41
ideals with factors being zero rings. Some further results
are given.
Card 2/2

FREYDMAN, P. A., Cand Phys-Math Sci -- (diss) "Rings of a solvable
type." Sverdlovsk, 1960. 8 pp; (Ministry.of Higher and Secondary
Specialist Education RSFSR, Urallskiy State Univ im A. M. Gorlkiy);
150 copies; price not given; bibliography at end of text (15 entries);
(KLI 17-60, 140)

14-1300
AUTHORt -Preydman, P.A.
89033
S/044/60/000/009/003/021
CIII/C222
TITLEs On Rings With the Idealizer Condition
PERIODICALs Referativnyy zhurnal. Matematika, 1960, No-9, P-33,
Abstract No.10080. Uch.zap.Urallskogo un-ta, 1959, vyp.23,
No.1, pp-35-48
TEXT% The author investigates rings with the idealizer condition, i.e.
rings in which every proper subring is different from its idealizer
(the idealizer of a eubring Q in the ring K is the greatest subring of K
in which Q is a two-sided ideal). In a certain sense, the rings with the
idealizer condition or briefly U-rings are a ringtheoretical analogue of
the groups with the normalizer condition. Basic results: 1) A ring K is a
U-ring generated by one element if X in a direct sum K - P+Kj , where
P - C/(m) (C - ring of integers, m 0), while Ici is a ring generated by
a single element b so that b 6+1- b - 0 for a certain integral K, where
m divides a certain power J1 of (he number r.
2) The ring K is a U-ring with minimal condition for two-sided ideals
then and only then If K is a direct sum X - P;R , where P - CAM) W 0),
while R is a nilpotent ring with minimal condition for two-sided ideals.
Card 1/2

a
$104Y6010YRO910031021
0111 c222
On Rings With the Idealizer Condition
3) The ring X is a U-ring without nilpotent elements being different
from zero then and only then if K is isomorphic either to the discrete
direct sum of the fields C/(p ) (pi - different prime numbers) or to
a ring generated by an integel -f~ 0, or to the direct sum P;kj, where
P - C/(m) (m~ o,�1 and free of squares of prime numbers) and K1 is a
ring generated by the integerCj 01 where m divides the number f.
From the last theorem it follows that in a U-ring without nilpotent
elements being different from zero every subring is a two-sided Ideal.
[Abstracte-'s note: The above text is a full translation of the
original Soviet abstract.]
Card 2/2

FRL'YDI,W',
p P.A. (Sverdlovsk)
-
RLngs, all. subrings of which ar-2 metaiden.19 of a finite in(lex.
Hut. sbor. 65 no.301.5-32.3 11 164 (IMA 18tl)

FREYD14AII"P.A.
: - - -'-. -.. " I-
Some finiteness conditions in associati7e ring3. !.Iji*,. zap.
Ural. mat. ob-va UrGu 3 no.1:77-84 161.
19:1)

FRIM". S.L.; SMMV, K.At, profeasorp zavediiyushchiy.
bow,
Iffect of prolonged sleep upon the development of adIpose dystrophy in
rabbits poisoned by phosphorus. Farm.i toke. 16 no.1:22-24 Ja-F 15).
(KI-RA 6:6)
I.Laboratorlys, kafedry farmakologii Saratovskogo meditsinskogo instituta
(for Freydman). 2. Kafedra farmakologii Saratovskogo ineditsinskogo Insti-
tixta (for Shmelev). (Sleep) (Dystrophy) (Phosphorus--Physiological
effict)
Prolonged uninterrupted sleep produced by berboWl nodim
anvUl is capable of reducing considerably diaturtances of metabolism which
arias in rabbits as a result of P poisoning. These distufoances lead to
acc=ulation of fat and water in organs,
254TU

SHERISHCRINA, S.I., PONOMAREVA, 0.1., FREMLAY, S.L.
Inolntion of Leptwipirn in thick media. Lab.delo 4 no.3:46-47
My-ja 158 (MBU 11:5)
1. Iz knfedry mikrobiologii (zav. - prof. S.I. Sherishorina)
Sarntovakogo meditsinskogo instituta.
(LEPTOSPIRA)

BYRZM, P.J., prof.; VAESHMOV, L.A., prof.; VOLYBSKIY, B.G., dotsent;
(ZHA IMOV, N.V., dotsent; GURNTICH. L.I., dotsent; ZHELYABOVSKIT,
G.M., prof.; XARTASHOV, P.P., prof.: 1OCHETOV, X.P., dotsent;
UtUGLOV, A.Y., prof.; WMIN, M.P.. prof.; LARINA, V.S., dotsent;
LOW, I.S., doktor (deceseed]; LUKOVA, A.Io, prof.; HAKHLIN,
Ye.Yu., prof.; NAUMOV, A.I., kand.med.nauk; POPOVITAN, I.M., prof.;
SOLUN, N.S., kand.med.nauk; TARABUKRIN. X.M.. dotsent; THIT'TAKOV,
K.N., prof.; TRISHINA, A.A., lmnd.med.nauk; ULIYANOVA, A.V., dotsent;
TAY9. A.B., kand.med.nauk; FAKTOROVICH, A.M., dotsent; FRANKFURT,
A.I.. prof.; VISHZR, L.I.. dotsent; CRASOVNIKOVA, Ye.1'.. kand.mod.
nauk; SHAKAM, P.I.. prof.; SHAPIRO, M.Ya., dotsent; WARTS, L.S.,
prof.; SHUSTERKAH, I.B., dotsent; FOY, A.M.. prof.;-ZESMw-1 -S-L-9-
kand.med.nauk; NIKITIN, B.A., dotsent. red.; AFANASIYET, I.A..
red.; LUKASHEVICH, V.. tekhn.red.
[Concise medical reference book] Kratkii terspevticheskii spra-
vochni.k. Izd.3., ispr. i dop. Saratov, Saratovskoe knizhnoe
izd-vo. 1939. 919 p. (MIRA 13:7)
1. Chlen-korrespondent ANN SSSR (for Trettyakov).
(XIDICIM-HANDBOOKS, MANUALS, RTC.)

VOLYNSKIY, B.G.1 FREYDMANP S.L.; GLAZYRINAs, G.A.; KUZ'M1VAq K.A.;
KUZIIETSO~,~-t'-$-.~.2;--GVOZDnV, A.V.
Use of vitamins in some toxications under experimental conditions.
Trudy Bar. goo. med. inst. 26:119-121 159. (MIRA 14:2)
1. S,aratovskiy meditsinskiy institutp kafedra farmakologii
(zav. - dotBent, B.G. Volynskiy).
(POISONS-PHYSIOLOGICAL EFFECT)
(VITAMIN THERAPY)

VOLYNSKIYI V.G.; FRZYDHANy_g,.~KUZNETSOVA, S.G.; KUZIMINAp K.A.;
GVCZDKOV, i-.-V~'
Influence of vitamin B12 on the course of experimental phospborus
intoxicatione Trudy Bar, goso mede inst. 26:122-125 159,
(14IRA 14:2)
1. Saratovskiy meditsinskiy institutj, kafedra farmakologil
(zav.- dotoent B.G. Volynskiy).
(CYANOCOBALAMINE) (PHOSPHORUS-TOXICOloOGY)

-- -FREYDMANp S.L.
Metabolism of nucleic acids and nucleoproteins in infectious
hepatitis and in experimentai phosphorus intoxication.
Trudy Sar. gos. med. inst. 26:132-134 159. (MIRA 14:2)
1. Saratovskiy meditsinskiy institutq kafedra biokhimii (zav.-
prof, N.N. Ivanovskiy) i kafedra farmakologii (zave - doteent
B.G. Volynskiy).
(NUCLEIC ACIDS) (NUCLEOPROTEINS) (HEPATITIS, INFECTIOUS)
(PHOSPHORUS-TOXICOLOGY)

FOY, A.M.; VOLYNSKIYp B*G.; IVAIIOVAq V.V.; MYDMANp S.L.
Antiemetic action of some derivatives of the phenothiazine
aeries. Trudy Sar. gos. med. inst. 26:167-174 159.
(MIRA 14:2)
1. Saratovskiy meditsinski7 institutp akusherskc-ginekologichesRaya
.klinika lechfake. (zav.prof.A.M. Foy) i kafedra farmakologii
(zav, dost. B.G. Volynoldy).
(PHENOTHIAZINE) (VOKITING)

ANDRYUSHECHKINA, A.V.; NIKOIAYEVAp L.P.; FREMIAN2 S.L.
Colorimetric method for tho determination of desoxyribonucleic acid
in the tissues of animals and in the cells of microoyganisms.
Lab. delo 7 no.1s7-8 Ja 161. (MIRA 1-4: 1)
1. Kafedra biologicheakoy khimii (zav. - Prof. N.N. .1vanovskiy)
i Kafedra farmakologii (zav. - dotsent B.G. Volynskiy) Saratovskogo
meditsinsko o instituta.
NUCLEIC ACIDS) (COLORMTRI)

SHERISHORJNA, S.I.'; VOLYNSKIY, B.G.; MOROV, N.N.; FREYDMAN, SIL.j PONOMARWA,
0.1.
Furacillin and levomycotin therapy for patients with cystitis,
Urologiia 26 4o.2:27-~2 161. WIRA 14:3)
(BIADDER-DISEASES) (OMYCE-TIN) (FURAN)

VOLYNSKM B.G.; FREYDW, S.L.; BENDER, K.I.; KUZIHIFA, K.A.;
KUZNF.TSOVr,'SO'G.; MARTYWOV, L.A. (Saratov)
Prevention and treatment of radiation siclmeas in an experiment.
Med,rad. no*9:81 161. (KIRA 15:1)
(RADIATION SICUMS)

FURSIAYEV, A.D., zasl. dayatell nauki RSFSR, doktor biol. nauk
(deceasedl; VORONINA, K.V.; VOLYNSKIY, B.G., kand. med.
nauk; FREYDMAN, S.L ; BENDER, K.I.; KUZIMINA, K.A.;
MARTYNOV, L.A.; KUZNETSOVA, S.G.; VINNIKOVA, I.A., red.;
ZENIN, V.V., tekhn. red.
(Medical plants and their utilization in medicine] Lekar-
stvennye rasteniia i ikh primenenie.v meditsine. In.p.]
Izd-vo SarRtovskogo univ., 1962. 202 p. (miRA 16:6)
(BOTANY, MEDICAL)

VOLYNSKIY, B.G.; BiIDEV, K.I.; 1 4
S.L.; kINTMOVA, A.,
rod.
[Frescription manual; textbook for physicians anA stu-
dents] Retsepturnyi spravochnik; po!;obie d1la i
studentov. Izd.2., dop. i perer. Sarptuv, Sava-
~v
tovskogo univ., 1964. 206 p.

ACC N I, CODE, : t]R/0417/66/000/010/0002/0002
A10000600 f"~V) SOURM
AUTHOR: Volynskly, B. C. ; Bender, K. 1. ftqy4man, S. L, Ruznetsova,
S. G. L. A.; Bogoslovskaya, S. 1.
TITLE: Reaction of the organism to drugs during hypothermia
SOURCE: Ref. zh. Farmakol, khimiotcrapevt sredst, toksikol, Abs. 10. 54, 4
REF SOURCE: Tr. SAratovok, rned. in-ta, no. 40(66), 1966, 194-107
TOPIC TAGS: hypothermia, drug, respiratory drug, rabbit, reaction rate, blood,
cardiac activity, tissue metabolism
ABSTRACT: The effects of some drugs on hemodynamics, respiration and tissue
inctabolism was studied in mice, rats and rabbits cooled to 19-20C. Caffeine
(10 mg per kg) and euphyllin (4. 8 mg per kg) have caused a stable decrease of AD
and have depressed the tissue metabolism levels (the quantity of glycogen, ATP
and electrolytes). ' Cordiamin (25 mg per kg) has also depressed tile AD and inter-
fered with the respiratory and cardiac activity. Lobeline did not affect the
respiration. Bernegride and KM have lowered the AD and sharply inhibited
Card 112 UDC: 615. 1

-46C-10
AR7000600
respiration. The effect of adrenaline and mesaton (0. 1 mg per kg) on respiration
and AD did not vary. Morphine (1 mg per kg) did not contribute to an increase of
inhibiting effect of hypothermia on respiration and blood circulation. Hypoglycemil
effect of insulin and spastic effect of strychnine and camphor was found to be
weaker during* hypothermia, A. Novik. [Translation of abstract) [AM]
SUB CODE: 06/
Card 212

YR22MAN. S.M. XiaASHNIXOVA, V.S., redaktor; TJRESHGBNNKO, I.I.. redaktor;
TXSXOVA'- tekhnicheskiy redaktor
[Gollective farm directorls manual] V pamoshch' predsodateliu. kolkhoza.
Moskva, Goo. izd-vo selkhoz. lit-ry. 1956. 411 p. (L)Ikhozaaia
okonomichooknia bibliotechka. no.2) (MIRA 10:1)
(Gollective farms)

y I ZI L- I p CIO*% -f-~ -I'S . kn .
BKLYAVSKIY. A.V.; BANNIKOV, N.A., red.: YRNYI)KAN, S,M., red.; SOKOLOVA, N.M.,
tekhn.red. ----
[Heroes of socialist fields] Geroi sotsiAllstichaskikh polei
(1917-1957). [Moskva] Goa.tud-vo sellkhoz.lit-ry, 1957. 630 P.
(Agriculture)

KORSAKOV. Ivan Yefimovich; MsYDKAH, S.M., red.,- SMIRNOVA, Ye., tekhn.red.
(Economic calculationn on a collective form] Ekonomic:aeakis
raschety v kolkhoze. Moskva, Goo.izd-vo sellkhoz.lit-:ry, 1958.
73 P. (HrRA 12:9)
(Collective fame--Accounting)

TSIBIM, Konstantin Tovataflyevich, qaroy Sotsialisticheakog-o Traa;
YRAIDW, S.K., red.; DBTIffA, F.M., tekbu. red.
[Second year without the vorkdiLy system; practices of the wBol&evlko
Collective Parng OW Frovimm, Ukraine] Vtorol god b-9z tradadnla;,
opyt kolkhosa "Bollshavikw Stimokot oblanti Ukrainskoi SM Nookw&,
Gba. izd-vo selikhos. lit-ry, 1958. 16o p. (MIRA nsIO)
(Collective fame) (wages)

SAPILINIKOV, Nikolay Georgiyevich, kend.ekonom.nai*; FRETIKM, 3,K,, reds;
BACHURINA, A.M., takhn.red.; PROKOFIYEY.A, L.Y.. tekhn.red.
(Economics of cotton growing on collective formal Iconomika
khlopkovodetva v kolkhozakh. Kookva, Goe.izd-vo sel'khoz.lIt-ry,
1959. 335 P. (MIRA 13:4)
(Cotton growing--Costa)

TIRNA A, U.S., doktor skonom.nauk, red.; KOTOT, G.G., red.;
OBCLENSKIT, X.P., red.; ZASEAYSEATA, T.I., red.; FRETDW, S.M.,
red.; YBDOTOYA,A.P., takhn.red.
(Labor productivity In socialist agriculture] Proizvoditellnost'
truda v sotsialistichookom sellakom khoziaiatva-, voprosy metodo-
logii i metodiki. Koskva, Gos.ind-vo sel'khoz.lit-ry, 1959. 422 p.
(Mm 13:3)
1. Akademlys nauk SSSR. Institut ekonomiki. 2. Intititut ekonomiki
AN SSSR (for Karnaukhova).
(Agriculture--Labor productivity)

KROKHAL , Podor Sergeyevich. doktor ekonom.nauk; KABTOROVICH, A.V.,
red.; 7RZTDKAN, S.K., red.; MWAR, V.I., tekhn.red.
(Outline history of farming systems] 0 sistemakh zem.-ledeliio;
iotorichaskii ochark. Koakva, Gos.izd-vo selikhO2.lit-ry. 1960.
430 p. (KIRA 13:12)
(Agrieulture)

BELOUSOT, TV.A.; KORCHAJODY, A.T.; RUDINEKIT. TeJe.; %WNOVA, Te.T.;
BANNIXOT. N.A., red.; ZAPITAKHM, A.I., red.; LAPIDUS, N.A.,
red.; RAKITINA, Ye.D., red.; IMSHCHMO. N.1., red.; FRIIIINAN,
-S.K,, red.; BALLCOD, A.I., takhn.red. . . . ........I
[Manual on ru"l subsidiary anterprioes] Sprimochnik po, sel'skim
podsobays predpriiatiiam. Kaskya, Goe.izd-vo sellkhot.lit-ry,
196o. 798 P. (NEU l3t12)
(Manufactures) (Form produce)

CHESHKOV, Aleksandr Fedorovich, kand. ekonom. nauk, starshiy nauchnyy
sotr.; EREV-DIIXI S M., red.; TRUKHINA, 0.11., tekJ3n. red.
(Integrated
mechanized brigades and teams] Kompleksnye me-
khanizirovam3ye brigady i zvenlia. Moskva, Izd-vo sellkhoz.
lit-ry, zhurnalov i plakatov, 1961. 133 P. (MIRA 15:4)
1. Vseaoyuzmyy nauchno-issledovatellskiy institut ekonomiki
sellskogo khozyaystva (for Cheshkov).
(Farm management)

MELINIKOV, Ivan Gerasimovich; FREYDMAN~ S.M., red.; SOKOIDVA, N.N.,
tekhn. red. I--.- I-- ~ ~ - -1- --------,
(Possibilities for improving the quality of agricultural production)
Rezervy povysheniia kachestva sellskokhoziaistvemoi p-roduktsii.
Moskvao Izd-vo sallkhoz. lit-ryp zhurnalov i plakatov., 1961. 166 pe
I (MIRA 14:11)
(Farm produce)

HASKINI G.F., kand. sellkhoz. nauk; VAY111i, 1`~.G., kand. sellkhoz.
nauk; YEREVIEYEV, K.I., kand. okon. nauk; ALIMIYEV, V.P.,
kand. ekon. nauk; GOLENKO, M.V., mlad. nauchn. sotr.;
GANZIIA, N.M., PLIad. nauchn. sotr.; F4~LTDWZ, red.;
MAKHOVA, V.N., tekhn. red.; TRUKIIINA, 0.11.1 te hn. red.
(Efficiency of capital investments in agriculture] Ef-
fektivnost' kapitallnykli vlozhenii v sel'skoe khoziaistvo.
Mo.-kva, Sel"yhozizdat, 1963. 294 p. (1,11RA 17: 1)
1. Moscow. Vsesoyuznyy nauchno-issledovatel'skiy institut
ekonomiki sellskogo khozyaystva. 2. Dauchnyye sotrudniki
V.,iosoyuznogo naucluio-issledovatellckogo instituta ekonamiki,
soltokogo khozyaystva (for Raskin, Vayner, Yeremeyev,
Allferlyev, Golenko, Ganzha).
(Agriculture--Finance)

FIZEIDMAN'
(EffiCient 11DO Of t]7--'-' lllr,~ilj 1~;Tcllz-.-.r--r,-~-,~
zerili. Moskvri, sollkhozizdat, p.
(MII?A .18; r~)

PERINYKIN, Vasiliy Illich, kan(:. sc.,Ilklioz. nauk; DVORYADKIV,
V red.;
Ilikolay Ivhnovich, kar,---. ekon. nauk;
DOZLOVSKAYA, MI.D., teklin. red.; OKOIXLOVA, Z.F., tekhn.red.
[Econor-ics of oiloeed plant production) Ehonordka proiz-
vodstva raslichnykh kulltur. Vuslrva, Scllk~ozizdat) 1963.
346 p. (maA 16:U)
(Oilseed plants--Economic aspects)