SCIENTIFIC ABSTRACT KOMIN, A.V. - KOMISSAROVA, L.N.
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USSR UDC 535-343.1
SOLUKhIN, R. I., YaKOBI, Yu. A. ar4j9ft1,N,_Aj, Y.,, Institute of Theoretical and
Applied Mechanics, Siberian Branch of the Academy of Sciences of the USSR
"Discussion of Some Results of the Calculations"
Optichesklye Kharakteristiki Vodorodnoy Plazmy, Novosibirsk, t'Nauka,, (Siberian
Branch), 1973, PD 40 - 48
Abstract: The SDecial characteristics obtained are based on modern theoretical
concepts and do not require extensive commentary. A few interesting results may
be noted. At a temperature of 0.6 electron:yolts the Doppler mechanism begins to
predominate for the la and LO resonance lines at I atmosphere and for the In lines
at 10 atmospheres. because of the low electron density at this temperature and the
deen locations of the levels correSDonding to these lines, At 10 and 20 atmos-
pheres, the lines are clearly visible ejrainst the backgroundl at high temperatures
they become narrower again because of the reduced electron density.
Although much energy is in the Lyman lines and continuum, self-absorption
reduces radiation in these regions quite strongly, particiLlarly at low tempera-
tures.
The lines of the Balmer and Lyman series tend to fuse even at relatively
low quantum numbers. There is some question about the boundary between discrete,
113
USSR
SOLMIN, R. I., et al., Opticheskiye Kharakteristiki Vedorodnoy Plazr,.y, 1973,
pp 40-48
continuous spectra and the relative displacement of this boundary due to Cculamb
interactions and the smearing of lines as a result of transitions frora high energy
levels. The authors' calculations show that the spectral lines begin to fuse
significantly earlier than the Coulomb "trimming" of the discrete spectrt,41.
In addition to the spectral curves, the authors calculated integral
energy losses for hydrogen plasma over the range of parameters used. Special
calculations were made to relate their work to that of D. 13. 01fe, reported in
J. Quant. Spec. Rad. Trans. 1,104, 1961, and satisfactory agreement was found.
The use of lasers to probe plasma requires quantitative information
about the relationship between transparency and plasma tarperature and density.
These calculations were performed in two vays, as-sixi-iing constant proosir.-(:, and
at a given initial particle density. The first procedure'is neceroary bc!cause
the plasma has significant abqorption only at relatively high pressures, yielding
a condition without significant pressure gradients, but with high tempercture
and density gradients as the plasma is forced agains-t the, walls. Although there
is an overall tendency toward absorption at longer wave lengths, there are
anomalies due to the existence of strong absorption lines which are more or less
active, depending on pressure and temperature. The second forn of calculation
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UOSSR
SOLUMN, R. I., et al., Opticheskiye Kharakteristiki Vodorodnoy Plazmy, 1973,
pp 40-48
is more appropriate when the laser beam is directed along the long axis of the
plasma chamber, as well as in evaluating the transparency of a plasma under
laser heating.
313
PHYSICS
Electricity & Magnetism
USSR
LOBANOV, K. M., and USTYUZHANINOV, V. G.
"Effect of an Electric Field on Particle Movement in a Stellarator"
Leningrad, Zhurnal Tekhnicheskoy Fiziki, Vol 40, No 7, 1970, pp 1,346-1,350
Abstract: The equipotential surfaces of the electric fiald in question in this
article coincide with the magnetic surfaces of the stellarator. The method
followed by the authors in making their calculations is to solve, by the Runge-
Kutta method, the system of differential equations describing the motion of
charged particles in the electric and magnetic fields. These equations are
given in vector form. Since the exact analytic exprearion for the magnetic
surfaces is unknown, the averaged magnetic surfaces ~!xpar:hnenLally corrected
in the separatrix region to reduce the divergence betweei~ the true and equi-
potential magnetic surfaces are used. The results of the computations indicate
that the electric field strongly affects the particle trajectories. The authors
express their gratitude to R. Z. Sagdeyev and A. A. Galeyev for thier useful
cominents.
USSR UDC 535-310.1
SOLUKhIff, R. I., YaKOBI, Yu,.A., and NOMIN, A. V.v Institute of Theoretical and
Applied Mechanics, Sib~rian Branch 6f th6-Abddemy of Sciences of the USSR
"The Continuum"
Opticheskiye Kharakteristiki Vadorodnoy Plazmy, Novosibirsk, "Nauka"
(Siberian Branch), 1973, pp 23 - 29
Abstract: Continuous spectra are generated by transitions to, from, or within the
unbound- (n free") state. At temperatures below 5000 degraos these represent
free atoms (the total continuous radiation is small) while at higher temperatures
free electrons are a primary radiation mechanism. At elec,,.ron temperatures much
less than 500 ev a semiclassical treatment is appropriate, yielding the so-called
Kramer's foriulas with the Gaunt factor as a quantum mechanical coi-rective. A
formula for recombination radiation can be obtained by applying Kirchhoff's law
for local thermal equilibrium to the formulas for photo-toniZatiDll absorption.
This radiation is chara~fterized by significant intensity close to the line series
and an exponential decay in the direction of short vave:s. Brensatz-abluni7z, extends
Indefinitely in the direction of long waves. The ratio of these two effects can be
calculated for a riven temperature and frequency, AnotheT, factor is so-called
multi-quantum recombination occurrim5 as a result of' triplo recombination. In a
nonequilibrium plasma this can substantially influence the distribution of electrons
in levels and the number of free electrons, but in an equilibriut plazma a
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U-5SR
SOLUMIN, R. I. et al, Opticheskiye Kharakteristiki Vodorodnoy Plazmy, Novosibirsk,
"Nauka- (Siberian Branch), 1973, pp 23 - 29
Boltzmann distribution in the levels is established, uniquely determined by 0
temperature equilibrium. At fairly high pressures and temperatures below 10,000 K
a significant role is played by the frurmation of ne.gative hydrcgen ions,
accompanied by radiation. At still lower temperatures continuous molecular
spectra appear. There is also the so-called quasi-molecular continuum, which Is
due to the transition of a hydrogen molecule from an initial unstable state
(occurring as the result of a collision betveen atoms with parallel spins), to a
stable state.
In addition to the true continuumt there are quasi-continua, resulting from
the overlapning of large numbers of broadened lines. '1hese occur as various
bands. At temperatures below IOOGOX,. induced rotational transitions are signifi-
gh the radiation of gases at low temperatures is vent low, the
cantl althou,
coefficient of absorption is quite significant.
2/2
14
UDC 535.343.1
SOLUKhTJT, R. I., YaKOBI,.Yu. A,, an'~Xoml,,.-A....V., Institute of Theoretical and
Applied Mechanics, Siberian Branch of the Academy of Sciences ofthe USSR
NSpectral Lines"
Optiches;dye Kharakteristiki Vodorodnoy Plazmy, Novosibirsk. "Nauka
"Siberian Branch), 1973, pp 16 - 23
Abstract: Three factors determine the nature of spectral linesi population,
transition probabilityand form of the line. Although many processes contribute
to population distribution, collision with electrons and spontaneous radiation are
usually dominant. At low plasma densities secondary collisions can be ignored and
radiative transitions are dominant, while in dense plasmas nonraliative de-excitation
predominates. When the electron density becomes sufficiently high, radiation
intensity becomes independent of Itj the plasma becomes a Bol-tzmann radiator.
Spectral lines from a plasma are all broadened as a re,,ult of Interaction -with
fluctuating internal microfields. The extension can be considered in termns of two
components: one described as the result of a lineax Stark effect due to the inter-
action of Ions with other, relatively slow ions, and the other due to collision
broadening, (also with a Stark effect component) from interactions with fastei-movin--
electrons. The electron effect is most significant at the center of the broadened
line, the statistical effect )at its edges, Tho center is also somewhat displaced
1/2
USSR
SOUMB, R. I., et- a-1., ODticheskiye Kharakteristlki Yodorodnoy ?lazmy, Novisibirsk,
"Nauka- (Siberian Branch). 197j, pp 16 - 23
from what would be obtained from an isolated atom. Alt-hough theoretical calculations
for the edges of the broadened line show good agreenent with experiments, computations
for the central Dortion are considerably less satisfactory. In this area the
authors.base their work on a theory developed by Sobellman, exte-nded to cover also
broadening due to collisions with other particles,
When the concentration of charged particles Is low, Doppler broadening becomes
significant. The integral exDression for combined Do-apler and dispersion broadeniR-,
is not in finite form, so that calculation by approximation method is required.
2/2
_1jSSR*%
UDC 535.343.1
SOLUMAN, R. I., YaKOBI, Yu. A., and KOMIN, A, V., Institute of Theoretical and
Applied Mechanics, Siberian Branch'"Of""the-Academy of.Sciences of the USSR
"Method of Performing, the Calculations"
Opticheskiye Kharakteristiki Vo-dorodnoy Plazmyp Novosibirsk, "Nauka" (Siberian
Branch), 1973, PP 33 - 39
Abstract: Five mechanisms vere considered in the computer programs used:
1) bound-bound electron transitions (linear radiation from atoms); 2) free-free
and free-bound electron transitions in the field of protons (the H continuum);
3~ free-free and free-bound electron transitions In the field of atom_-(H-coxitinuum);
4) free-free and free-bound proton transitions.in the field of atoms (the H' 2
continuum)i 5) continuous radiation of quasi-molecular hydrogen
(Hquasi2 continuum). Previous studies have lumped line spectra In two or three
groups. The present work considers all transitions between discrete levels in the
hydrogen etom that realis'Llically exist in the plasma. Within the limits of the
paxn.meters chosen, this nLn-be,- varies from less than 10 to several tens of levels;
the number of snectral lines is proporttional to the square of this number, Each
line is considered in its broadened form. The results are presented on a wave scale.
Variable step sizes are used to keep the calculation error approximately constant
over the entire spectrum. Step sizes were based on relative values of the deriyative
1/2
'USSR
SOLLMIN, R. I., et al., Opticheskiye Khar-akteristiki Vodorodnoy Pla2my, Novosibirsk,
"Nauka" (Siberian Branch), 1973. P? 33 39
of siDectral intensity, except where the contribution of the raximum line was less
than 1/10 the background radiation, where the step size was based on the continuum.
In each, step the calculation of step size was based on the line making the
strongest contribution, rather than the 31ne with the nearest center.
The program was written in ALPIIIA, a modification of ALGOL. Calculations
vere performed at the computer center of the Siberian Branch~ Academy of Sciences
of the USSR.
2/2
USSR UDC 535-343.t
SOLUKhIN, R. I., YaK6BI, Yu. A., and KOMI-1,...A...-V..,-Institute of Theoretical and
Applied Mechanics, Siberian Branch ol'- ihe Academy of Sciences of the USSR
"Energy Structure of the Hydrogen Molecule"
Opticheskiye Kharakteristiki Vodorodnoy Plazmy, Novosibirsk, "Naukall
(Siberian Branch), 1973, pD 12 - 14
Abstract: Quantum mechanical analysis shows that the diatomic hydrogen molecule
is not stable unless the ends of the two electrons are In an antiparallel
orientation. Althouah the two electrons of the molecule can be in various
enerry states, they are within an axially symmetric field whose axis of syra-,etry
Is the line connectim-, the two nuclei. In this case what is significant is not
the absolute value of the orbital moment. but Its projection on the axis Xl;,
where 'K is Planck's constant and I is a quantum number similar to the
magnetic quantum number m in atoms.
In addition to the electron degrees of freedom, the molecule has oscillatory
and rotational de,~~rees of freedom. For each characteristic electron state, there
is a set of discrete oscillatory states, wbich can be obtained as the solution
of Schroedinger's equation for a harmonic oscillator. Cartsiderntion of lion-
h rmonic oscillations leads to a more complex expression. Rotation is also
1~2
-USSR
SOLUKUH, R. I., et al., Oiticheskiye Yharakterlstiki Vodorodnoy Plazmy,
Novosibirsk. "Nauka (Siberian Branch), 1973, pp 12 - 14
characterized by a discrete selection of energy states, describable in terms of
the rotational quantum number, the molecular constant,anti a coefficient which
characterizes the relationshiD of rotation to oscillation (nonrigidity of the
rotator). Since the hydrogen molecule does not have a constant dipole moment.
it cannot in isolation have oscillatory and rotational transitions, but in a
real gas this prohibition is removed because of induced alectric, dipole moments
occurring in collisions. Althoi4gh any transition can occur, transitions of � 1
are most com:mon. For electron-oscillatory spectra, the relative probability of
various transitions is determined by the Franck-Condon principle.
2/2
USSR UDC 535-343.1
_Jnstitute of Theoretical xid
SOLUKUN, R. I., YaKOBI, Yu. A., and KOMIN,, A.
Applied Mechanics, Siberian Branch of t~~-X~~aemy of Sciences of the USSR
"Total Radiation from Hydrogen at Temperatures Below 10,000 Degrees"
Opticheskiye Kharakteristiki Vodorodnoy Plazmy, Novosibirsk, "Nauka" (Siberian
Branch), 1973, pp 29-33
Abstract: Calculating the radiational characteristics of gases at relatively
low temperatures requires primarily consideration of molecular radiation.
Detailed calculations for this were made by Olfe in lGd6l. For a thin layer of
plasma in which self-absorption can be ignored, radiation from rotational transi-
tions predominates up to 10000; that from oscillation-rotational transitions
between 1000 and 50000. At higher temperatures negative hydrogen ions and posi-
tive molecular ions appear, the former more signi-ficant by an order of magnitude
from 3000 to 10,OOOOK. At higher temperatures linear radiation becomes signifi-
cant. When the plasma is of significant density and thickness, the results must
be-adjusted to account for the varying degrees of absorption, at different fre-
quencies and by different mechanisms.
1A
50
VSSR UDC 535-343.1
SOLUKhIN, R. I., YaKOBI, Yu. A., and K014INI,A..V., Institute of Theoretical
and Applied Mechanics, Siberian Blanl~of the Academy of Sciences of the USSR
"Energy Structure of the Hydrogen Atom"
Opticheskiye Kharakteristiki Vodorodnoy Plazmy) Novosibirsk, "Nauka",
(Siberian Branch), 1973, pp 9-12
Abstract: Schroedinger's equation yields solutions only for negative values of
E for which
E = 2)T2me4 _R
n h2n.2 ~7
where n is a whole number and R is the Rydberg constant, m must be replaced
by MM
M+M
where m is the mass of the electron and M is the rrass of the nucleus, to account
for movement of the nuclear mass. Relativistic generalization of Schroedin-
ger's equation requires that azimuthal quantum nw~lbers be considered in addi-
tion to the primary number n. In the presence of an external field, the
V2
I
USSR
SOLUBBI, R. I., et al., Opticheskiye Kharakteristiki Vcdorodnoy Flazmy,
1973, pp 9-12
magnetic quantum number must also be considered (Zerman effect). However,
not all transitions described by this scheme are found in spectroscopic obser-
vation. According to quantum mechanics, the following t~-pes of optical dipole
transitions are possible: change in azimuthal quantum niumber -- + 1; change in
magnetic quantum number = 0 + 1; change in m, 0; change in internal quantum
number azimuthal + msj 0 + 1.
2/2
USSR UDC 535-343.1
SOLUKhIN, R. I., YaKOBI, Yu. A., and X-PMIN, A. V., Institute of Theoretical
and Applied Mechanics, Siberian Branch'~~t-tht"AeAdemy of Sciences of the USSR
"The Composition of Hydrogen Plasma"
Opticheskiye Kharakteristiki Vodorodnoy Plasmy, Novosibirsk, "Nauka"
(Siberian Branch), 1973, pp, 5-9
Abstract: A plasma of pure hydrogen can contain ten different kinds of
particles -- H2 and H3 molecules, positive and negative ions of these molecules,
atoms, positive and niegative ions of the atoms, and free electrons. Diagrams
are given to show the relative contribution of each of these particles as a
function of temperature and pressure. The law of mass action gives the rela-
tive amounts of large particles and their breakdown products as functions of
the degrees of freedom of each such component. There are foL~r types of freedom:
electron, oscillatory, rotational, and translational. The product of the first
three is the statistical sum of internal degrees of freedom, called the statis-
tical weight of the particle. There are formulas for finding each of these as
the sum of a series in terms of energy of excitation, electron level, natural
oscillation frequency, oscillatory quantum number, and ather factors. Trans-
lational freedom can also be expressed in terms of mass and relative volume.
1/2
USSR
SOLMIN, R. I., et al., Opticheskiya Kharakteristiki Vodorodnoy Plasr%v,
1973, pp 5-9
Since dissociation and ionization ordinarily begin at temperatures
significantly below the corresponding binding energy, because cf the high
statistical sum of the free state, in the majority of cases only the basic
electron term need be considered and the unharmonic nature of hydrogen molecule
oscillations can be ignored. Several studies have deterinined ionization
energy in a plasma and its reduction due to the total-electric field of charged
particles around the atom, particularly Ecker and Kroell (10,63). The thermo-
dynamic calculations of plasmic composition made in the present work yielded
results close to those obtained by Fatah in 1969.
2/2
USSR UDC 535-343.1
SOLUKhIN, R. I., YaKOBI, Yu. A., and KOMIN, A. V., Institute of Theoretical
and Applied Mechanics, Siberian of Sciences of the USSR
"On the Thermodynamics of Radiation"
Optichoskiye Kharakteristiki Vodorodnoy Plazmy, Hovosibirsk, "Naukall
(Siberian Branch), 1073, pp 14-16
Abstract: The primary obstacle to establishing equilibrium in a system includ-
ing radiation is the loss of energy by radiaticn. outside the system. An
excited particle can lose energy either through a damping collision or by
spontaneous radiation. If there is any significant ionization, the majority
of collisions are with electrons. Thus, given.the damping collision cross-
section of the particle and its radiational lifetime (considering also stimu-
lated emission), the relative probabilities of damping and radiation can be
calculated. If damping is more probable, local thermodynr-mic equilibrium may
be established. Overall equilibrium will depend on the volume ab5orption
coefficient and the relative probability of damping. The calculations for
absorption must consider re-radiation, so that llabsorptic~111 -implies a sufficient
number of collisions to make the probability of damping high. If this tctal
path length is much greater than the dimensions of the volume, the result is
113
USSR
-SOLUKhT?I, R. I., e:6 al., Opticheskiye Kharakteristiki-Vodorodnoy Plazmy,
19732 pp 14-16
volume radiation; if it is much less, surface radiation. Fquilibrium radiation
of a surface plasma radiator is equivalent to that of an absolute black body
and is referred to as Planck radiation. Volume equilibrium in the sense of
local thermodynamic equilibrium yields so-called Boltzmann radiation, since the
nature of the radiation is determined by the Boltzmann di.-;tribution of electrons
in levels. While a special form of Kirchhoff's law applies to tYe latter case
and the black body radiation is determined from Planck's formula, nonequilibrium
radiation can be analyzed only by solving an enormous system of kinetic equa-
tions, since nature depends on the probabilities of a large number of elementary
processes.
In a moderately dense plasma local thermodynamic equilibrium is the
most probable state; it is sufficient for the probability of collision processes
to exceed the probability of radiation processes by an. order of magnitude. In
fact, the rigidity of this condition for a resonance transition with maxinram
probability of spontaneous radiation can be significantly reduced in the
majority of real- cases by the trapping of radiation in the optically dense
plasma. Since most experimental installations produce a plasma for a short
time, it is necessary to verify that the time to establish equilibrium is brIef
lil comparison with the time to establiah a quai;i-stable strAte. Thin can be
213
USSR
-SOLUKhIN, R. I., et al., Opticheskiye Kharakteristiki Vodorodnoy FlazMy, 1973,
PP 14-16
done by considering the slowest process, the relaxation of the resonance level.
Under experimental conditions, radiation scattering (primarily Thcmson
scattering) is ignored, since the mean free path is very long; under actual
physical conditions, this factor may be important.
313
16
4
USSR UDG 535-343.1
SOLMIN, R. I., YaKOBI, Yu. A., and KOMIN`,.,.A..V., Institute of Theoretical
and Applied Mechanics, Siberian BrahZK of the Academy of Sciences of the USSR
Opticheskiye Kharakteristik,4 Vodorodnoy Plazmy (Optical Characteristics of
Hydrogen Plasma), Novosibirsk, "Nauka" (Siberian Branch), 1973, 82 pp
Abstract: Results are given from detailed calculations of the special char-
acteristics of hydrogen plasma over a wide range of paxameters, considering.
all significant radiation mechanisms. The material on the computation is pre-
ceded by a brief systematic summary of information about the hydrogen atom
and molecule and the composition and thermodynamic and gas dynamic properties
of the hydrogen plasma. Radiation processes are covered in detail, including
radiation from nonisothermic plasma, which requires simultaneous consideration
of radiation and thermal conduction. In this connection, the results of the
calculations are discussed, recommendations for their practical. use are mde,
and some questions of the diagnosticss of hydrogen plaswi aro exrunlnod.
This material will be useful to a brond group of engincer-phys-ILcIsts
and graduate students and students in-senior courses specializing in spectro-
scopy, plasma physics, astrophysics, and physical gas dyaamiop.
1/3
USSR
SOLUKhIN, R. I., et al., Opticheskiye Kharakteristik; Yodorodnoy Plazmy, 1973,
82 pp
CONTENTS Page
Introduction 3
1. The Composition of Hydrogen Plasma 5
2. Energy Structure of the Hydrogen Atom 9
3. Energy Structure of the Hydrogen Molecule 12
4. On the Thermodynamics of Radiation 14
5. Spectral Lines 16
6. The Continuum 23
7. Total Radiation from Hydrogen at Temperatures Below 10,000 Degrees 29
8. Method of Performing the Calculations
33
9. :Discussion of Some Results of the Calculations /to
10. Optical Diagnostics of Plasma 48
11. Radiation of a Nonisothermic Plasma. Transfer Coefficl.ents 55
12. Radiation of a Quasi-Equilibrium Hydrogen Plasma, Considering
Conductive Thermal Conductivity 59
13. Gas Dynamic Properties and Kaments of Radiation Gas Dynaudics 61
14. Laser Heating of a Plasma 69
2/3
USSR
SOLMIN, R. I., et al., Opticheskiye Kharakteristiki Vadorcdnoy Plazmy,
- 82 pp
1
9732
15. The Role of Hydrogen Plasma Radiation in the Problem of
Thermonuclear Fusion 73
Appendix 79
3/3
USSR
UDC 535-343.1
SOLUh-hIN, R. I., YaKOBI, Yu. A.0 and KOMINI A. V., Institute of Theoretical 3nd
Applied Mechanics, Siberian Branch --_- f Sciences of the USSR
o the ca emy o
"Optical Diagnostics of Plasma"
Opticheskiye Kharakteristiki Vodorodnoy Plazmy, Novosibirsk) "Naukall
(Siberian Branch), 1973, pp 48-55
Abstract: Plasma characteristics (primarily the concentration and temperature of
various components) are determined from:active and passive optical analysis.
Passive methods, in which the plasma is illuminated by external sources, have
the advantage of causing less perturbation to the plasila tMn other sampling
techniques, although nonlinearities must be considered-when such strong light
sources as lasers are used.
The most developed methods are based on measurement of radiative and
absorptive properties, althoug action are also
.,h measurements of the index of refr,
used. Due to the complexity of optical processes in a plasma, the most widely
used method is to begin with rough measurements based an one of the basic
radiation mechaniens and proceed to more detailed analys'Ls. Although in z:omc
particularly clear situations this method is expedientt there are many ca-ses
in which the preliminary determination of the primary mechtinism is quite
1/3
USSR
SOLUKUN, R. I., et al., Opticheskiye Kharakteristiki Vodoradnoy Plazmy,
Novosibirsk, 1973, pp 48-55
difficult or even meaningless. In addition, the overw1heiming majority of
these methods assume an optically rare plasma; when sellf-absorption must be
considered, this analytical approach leads to very complex expressions. A
more general approach, ignoring only those components Vhose contribution is
obviously unimportant, is clearly necessary. The use of computer calculations
over a broad range of parameters provides this more general approach, serving
M
as a "mathematical experiment" to relate the results of different studies and
serve as a guide for future research.
The index of refraction is the foundation of another group of mrthods,
primarily interferometry and Schlieren methods. These methods can determine
the density and density gradient of a single type of particle when this type
has primary influence on the effects of refraction. The relative sensitivity
of these two methods depends on the effective radius of the plasma forzation,
the diameter of the focal point, the focal length of the lenses used in the
Schlieren method, and the wave length of light employed.
Primary attention is currently on the use of infra-red and x-ray-probe
wave lengths. infra-red is particularly sensitive to t,'-.e charged particle
components, including the electron continuum. Passive x-ray diagnosis = be
used in determining parameters of a high-temperature plasma along the discharoe
2/3
......... .... . .
USSR
SOLUKhIN, R. I., et al., Opticheskiye Kharakteristiki Vodomdnoy Plazmy,
Novosibirsk, 1973, pp 48-55
axis.
As a rule, the diagnostic methods produce information about the plasma
in a given element of the volume at a specific moment in titre. Local discrim-
ination is achieved usualiy by using the Abel transform and assuaing'axial sym-
metry of the plasma formation. Time discrimination is achleved by using various
types of time scanning. Optical analysis of hydrogen plasma is characterized by
four specific factors: 1) absence of a constant dipole moment; 2) relatively
high availability of electrons, so that the continuumin the initial stages of
ionization in doterminod primarily by radiation relatod to negative ions;
3) the Stark effect as a prinary determinant of the qwctral line broadening;
complete ionization at high plasma temperatures.
313
'USSR
UDG 535.343-1
IN,_A. V In'stitute of Theoretical
SOLMIN, R. I., YaKOBI, Yu. A., and_NQM 4
and Applied Mechanics, Siberian Branch of the Academy of Sciences of the USSR
"The Role of Hydrogen Plasma Radiation in the Problem of Thermonuclear Fusion"
Opticheskiye Kharakteristiki Vodorodnoy Plazmy, Novosibirsk, "Naukall (Siberian
Branch), 1973, pp 73-76
Abstract: In the majority of thermonuclear installations radiation is the
primary source of heat loss, since the times involved are too short for con-
vection 'Losses (particularly when viscosity is increased by a magnetic field),
and conductive heat loss can be ignored when the plasizuL is aeparated or dis-
tant-from the walls. For a deuterium-tritium plaam, thf., necassary conditions
can be achieved at temperatures over 5 kev, while for lAtre deuterium they
cannot be achieved at all unless the magnetic field is used only for thermal
insulation, not retention of the plasma, or measures are taken to reduce
radiation lo:-s (use of an optically thick plasma Dr rad.lation-reflectinIg
walls).
Quantitative information about radiation capacity of the plafMa M---Acs
it possible to determine the minimum power of a steady-state reactor and the
minir-um temperature of its center in the general case of combined heat transfer
1/3
USSR
SOLUKh1-fi) R. I., et al., Opticheskiye Kharakteristiki Vodorodnoy Plazmy, 1973,
pp 73-7
and radiation losses. Assuming the plasma is not separated from the wall and
"I
its lifetime is not limited by instabilities, the zone of maximum. brigI tness
will be a hollow cylinder at a temperature of several electron volts. Cal-
culations indicate a minimal temperature of about 7 ke-v at the center of a
reactor without magnetic field, using a 50% deuterium-tritium mixture. The
dimensions of such a reactor must be on the order of several kilometers and
the heat loads on its walls must greatly exceed the capacity of modern mater-
ials.
Calculations show that an equilibrium reactor vith a magnetic field
would not produce energy at the center sufficient to compensate losses at the
exterior due to the poor heat transfer properties of the magnetized plasma
and that reflecting shells would be difficult to obtain, since most of the
radiation is in the form of x-rays.
Since continuous operation is apparently impossible, attention is
currently focused on various short-term processes. One main line of research
involves the use of relatively long laser pulses for supplementary heating of
plasma in various magnetic containment devices, while a second line is
directed toward the use of very short-pmterful laser pulses to bring targets
2/3
USSR
SOLUKhDI, R. I., et al., Opticheskiye Kharakteristiki Vodcrodnoy PlazMY,
1973) pp 73--'16
to the threshold of useful fusion without auxiliary eontai=aent. Unfortuiiately
laser efficiencies at the wave length needed for thin second process are very
low. There is also work being done on acmbined fusion-fission mechanisms,
using the fusion to produce additional neiArons for Improved fission output.
USSR UDC 535.343.1
SOLUKhN, R. I., YAKOBI, Yu. A., and KOMINI__A~ V..) Institute of Theoretical
and Applied Mechanics, Siberian Bra.R~i-_o"_f'_the Academy of Sciences of the USSR
"Radiation of a Quasi-Equilibrium Hydrogen Plasma, Considering Conductive
Thermal Conductivity
Opticheskiye Kharakteristiki Vodorodnoy Plazmy, Novosibirsko "Nauka" (Siberian
Branch), 1973, pp 59-61
Abstract: Only conductive and radiant heat transfer are considered in this
book, although convective transfer is important in a number.of cases, because
convective heat transfer has not been adequately studied, either theoretically
or experimentally. There are, however# many.cases in which convective transfer
does not occur.
The relative contributions of radiant and convective heat transfer for.a
plasma without interior directed velocities can be dettrmined from the differ-
ential equation of radiation transport and the law of onergy conservation. If
the absorbed energy is much less than the radiated energy, the system of des-
criptive equations can be reduced to two equations; an expression for heat trans-
fer which determines the state of matter throughout the entire volume, and an
expression of radiation transfer which can be used to find the spectral density
of radiation. This occurs in an optically thin system dithout external
172
fn H.
USSR
SOLUMIN, R. I., et al., Opticheskiye Kharakteristiki Yodorodnoy Plazmy,
1973, pp, 59-61
radiation flows. A similar separation can be obtaine4 if the absorbed energy
is greater than the radiated energy, but the total abrorption of the radiation
flow throughout the entire volume is less than the flow of energy related to
heat transfer and is thus incapable of changing the temperature distribution.
Truly radiative transfer states also exist, described by the so-called diffilsicn
or radiant heat transfer approximations, Although the assmption that radiant
heat transfer exceeds conductive.transfer is correct in the overwhelming major-
ity of cases, there is a region in which this is not true.
2/2
USSR UDC 535-343.1
SOLUKhI11, R. I., YaKOBI, Yu. A., and KOMI.A. V., Institute of Theoretical
and Applied Mechanics, Siberian BRh4h'6f. th*e-&ademy~of Sciences of the USSR
"Radiation of a Nonisothermic Plasma. Transfer Coefficients"
Opticheskiye Kharaktaristiki Vodorodnoy Flazmy, Novosibirsk, "Nauka", (Siberian
Branch), 1973, pp 55-58
Abstract: In the presence of a substantially nonisothermic plasma, radiation
transfer is described with the aid of special coefficients, calculated, in turn,
from the spectral characteristics of isothermal plasmas. In an optically thin
layer, the divergence of radiation flow can be described by using modified Planck
coefficients, while an optically dense plasma is described by Rosseland's equa-
tion. In the general case of arbitrary optical density, the radiation transfer
is computed by using the so-called modified emission capacity, Uthough the
calculations are simpler for extremely thin plasmas in ithich lines predominate
or extremely thick plasmas in which the continuum is dominant, real situations
usually require dealing with the more complex calculations of intermediate cases.
1A
USSR UDC 535-343.1
SOLUKhIN, R. I., YaKOBI, Yu. A., and K=N.l-.A-, V., Institute of Theoretical and
Applied Mechanics, Siberian Branch ofthe Academy of Sciences of the USiR
"Laser Heating of a Plasma"
Opticheskiye Yharakteristiki Vodorodnoy Plazmy, Novosibirsk, "Nauka" (Siberian
Branch)# 1973, pp 69 - 72
Abstracts Laser heatin-, is one of the prq?osed methods of attainiw'~ a controlled
thermonuclear reaction. The necessary conditions are the opposite of those
necessary for optical analysis without perturbation. There axe varying difficulties
in this process. At low temneratures, there are n3ny energy-absorbing txansitions
to be passed throur,rh, and raaiation losses begin to be significant as the plasma
Is heated. At higher tomporatures, effective heating, iv also reduced by the
Increase in transparency of the plasma. The heating InU..;4~ be rapid to prevent loss
of heat to the walls and the development of instabilitiiis. Use of a solid or
liquid target, although it requires additional energy for meltinT and eva-)oration,
makes attainment of the Lawson criterion easier because of the high initial Dlasr.,--
densityl if evaporation takes place from all sides simult-aneously, a significant
compression factor can be added
only inverse bremnstraldung is effective for
At thermonuclear temperatures, 0
heating. For plasmas of moderate density (less than or eqUalLto 1()l cm-3).
1/2
USSR
SOLUKhM, R. I., et al., Opticheskiye Khaxakteristiki Vodorodnoy Plazmy,
1973, pp 69-72
infra-red lasers are significantly more effective, but short-wave lasers are
most effective for heating solid targets.. The decrease in the coefficient of
absorption at very high temperatures may be compensated by the inverse cyclotron
effect. Heat absorption may also-be increased by severa- new types of non-
linearities that have recently been reported.
2/2
USSR UDC 535-343.1
SOLMIN, R. I., YaKOBI, Yu. A., and,KO.IN,__A.-V., Institute of Theoretical
_P4
and Applied Mechanics, Siberian Branch of the Academy of Sciences of the USSR
"Gas Dynamic Properties and Elements of Radiation Gas D~namiosll
Opticheskiye Kharakteristiki Vodorodnoy Plazmy, Novosibirsk, "Naukall (Siberian.
~Branch), 1973, pp 61-69
Abstract: In many cases, gas dynamic properties of plasmas rmust be considered
along with radiative properties. The authors a--bitrari',,.y distinguish two
thermodynamic regions: a ) temperature less than 10 electron volts and pressure
less than 1 atraosphere -- radiation is not blocked and the pressure of the
photon gas may be ignored; b) a "black" plasma at high temperatures and den-
sities -- radiation energy and pressure must be considered. There are also
such cases as the propagation of shock waves with high radiation flow,in which
it is necessary to consider changes in the thermodynamic properties of the gas
ahead of the front due to absorption of the flow of advance radiation from the
hot gas behind the front. Knowledge of some thermodynamadc and gas dynamic
properties of low-temperature hydrogen plasma is therefore also necessary.
Where there 15 overall flow of matter in an optice.'Lly t1iin plasma, the
usual hydrodynamic equations must be supplemented by a radiazt, energy factor
which represents a volume energy source. For an optically thick body in which
the radiant heat transfer approximation holdo, the statat of the matter is
dqtermined solely by itt; optical properties, In other cases, as in the problem
1/2
USSR
SOLUKhRI, R. I., et al., Opticheskiye Kharakteristik-i Vedorodnoy Plaz.-,Y,
1973, pp 61-69
without material flow, a complete system of equations mist ba solved.
The equilibrium concepts used by the authors are applicable to quasi-
equilibrium processes, since the time to establish equilibrium between radiation
and matter is of the same order as the lifetime of the photon, which is
usually very much less than the characteristic times of hydrod.,rnamics, which
are equal to or less than the thermal velocities of the molecules. Of course,
the usual conditions of quasi-equilibrium, must be supplor-ented by a condition
that the radiation absorbed by matter in the time interval of interest does not
change the state of the matter.
USSR UDC: 681.332.155
ALEKSEYEVSKIY, M. A., GAL'PEIRIN, 14. P. 0-
Z.
"A Device for Interrupting a Multicomputbr System!'
Moscav, Otkrytiya, izobreteniya, promyshlennyye cbraztsy, tovarnyje znaki,
:No 5, Feb 71, Author~s Certificate-No 293242, Division G, filed 3 Mar 69,
published 15 Jan 71, p 164
Translation: This Author's Certificate introduces a dtwice for interrupting
a multicomputer system. The device contains logic circuits, comparison cir-
cuits, diodes, flip-flops, a search module for the "one" furthest to the left,
a cor=and number register, an interrupt register, priority register-j, pro-
tection registers and a synchronization circuit. As a distinguishing feature
of the patent, the functional possibilities of the device are extended by
connecting as many priority registers as there are corputers to the in-outs
of the comparison circuits, connecting the second input's of the comparison
circuits to the search unit for the "one" furthest to t0he left in the priority
registers, and connecting the outputs of the inhibit-enable flip-flops to
the third inputs of the comparison circuits. Sowx-- outputs of the comparison
circuits are connected to diodes between the Comm.-nd counten und the command
number register. The other outputs are connected throu~7,h a logic circuit
to. the terminate flip-flop. The outputs of this flip-flop are connected
1/2
USSR
ALMEYEVSh-IY, M. A. et al., bSSR Author's Certificate No 293242
to the search unit for the "one" furthest to the left in the priority regis-
ters, while the second input of the terminal flip-flop is con-viected throuGh
a 1ogic circuit to the outputs of comparison circuits for protection codes.
The inputs of these comparison circuits are 6onnected to the decoder of the
search unit for the "one" furthest to the left in the interrupt register,
and to the outputs of the interrupt register, protection registers, and
inhibit.-enable flip-flops. The second outputs of these conparison circuits
are connected through a logic circuit, the synchronization circuit P-nd the
initiate flip-flop to the search unit for the "one" fizrthest to the left in
the interrupt register. The output of the interrupt register is connected
to the input of the search unit for the :"one" furthest to tLe left in the
priority registers, and the other outputs. are ccnnected through diodes to
the computer command counters. The synchronization circuit is connected to
the inhibit-enable f-lip-flop for interruption of all computers.
2/2
61
1/2 029 UNCLASSIFIED PROCESSING DATL---300CT70
TITLE-OLTONATICN FAILURES UURING BLASTING -tl;-
AUTHOR-104)-DRUKOVANYYt M-F.t KOMIRY V.M.r LITVINt L.N.9 OBEREMOK, G.N.
,.-,:COUNTRY OF INFO--U5SR
145(2)o 56-9
Zli. L970v
DATE PUBLISHED--70
_SUBJECT AREAS-ORDNANCE
TOPIC TAGS-EXPLOSIVEr DETONATION* TRINITROTOLUENE, WATER, HEXOGEN9 SHOT
8LASTING
,-!:CCNTRGL MARKING-NO RESTRICTIONS
DOCUMENT CLASS-UNCLASSIFIED
:,PROXY REEL/FRAME--3003/6434 STEP NO-UR/0127/'70/llt5/002/0056/0059
CIRC ACCESSICN NO--AP0129659
029 UNCLASSIFIED [PROCESSING DATE--30OCT70
CIRC ACCESSION NO--AP0129659
ABSTRACT/EXTRACT--(U) GP-0- A6STRACT. SYSTEMATIC EXPTL. STUDIES WERE
DONE TO CLARIFY CAUSES OF DETONATION FAILURES DURING BLASTING. TNT AND
'GRANULIT AS WERE USED AS EXPLOSIVES.. EXPLOSIVE CHARGES WERE PLACED IN
~GLASS~ TUBES 3.5-4 M LONG AND 'OF IOO-i40- MM IN DfArli. FACTGRS CONSIDERED
INCLUDED: STICKING OF THE CHARGE; FORMATION OF VOIDS; CONTAMINATION OF
THE CHARGE WITH WATEkv DUST, GRANULESt AND PIECES OF ORE; PRESE14CE OF
WATER IN THE BLASTING HOLE; ETC. DETONATION FAILURES ARE 140T LIKELY TO
BE CAUSED BY VOIDS AND THE PRESENCE OF INERT CONTAMINANTS. THE PRESENCE
OF H SUB2 0 CAN CAUSE FAILURES IN THE CASE OF SOL. OR 1-1 SUB2 0 REACTIVE
~EXPLOSIVES. UNSTABLE EXPLOSIVES CAN THEN FORM A KIND OF INERT BARRIER.
TROTYL AND TROTYL HEXOGEN DETONATORS ARE EFFECTIVE AND RELIABLE EVEN IN
LOW WTS. (13-200 G); THEY MUST BE USED IN scmEwHAr LAJIGER AMTS. FOR
INITIATIUN UF DETCNATION OF H SW82 0 CONTAMINATEU EXPLOSIVES. THE MOST
FRECUENT FAILURES ARE DUE TO QUENCHING DF*13URNING OF THE DETONATION
CORDr WHICH HAPPENS i6HEN THE CORE OF4HE.COkl) IS MOIST. IT IS
RECUMMENVED THAT THE MOISTURE INSULATION OF DETONATION CARDS BE
INCREASED.BY'APPLYING AN EXTRA BITUMINOUS LAYER* FACILITY:
INST. GEOTEKH. MEKH.l, KIEV, USSR*
USSR
GOLITSM, B. M. and KOMISSARCHIN, H. G. Pbysiootechmical Institute, Academy
r
of Sciences, USSR, Le
"Mechanical Stresses in Films of the Solid Solution OiSb),Te,"
Leningradq Fizika, Tverdogo Telap Vol 15, No It Jan 73P PP 301-303
Abstractt An investigation is made of mechanical stresses In films of an
extensively used thermoelectric material, the solid solution (BiSb)?To and
. 3P
the influence of these stresses upon conductance and the thermo-emf coefficient
Is evaluated. The stresses acting in the films were evaluated on the basis of
flexure of the backings. It was established that the films are in a stretched
state, the radius of curvature R of the backing comprising 6-7 zim. Calculations
conducted on the basis of a formula for determining tho stxvsses in the film#
show that considerable stresses are present in f-Ums with a surplus of tellurium
and in fIlms of stoichiometri-c composition; these stresses attain values of
25 kg/am4. Subsequent annealing of the films in an atmosphere of spectxally
pure argon at a temperature of 3aOoC brings about a decrease in the rad Ps
of flexurej, and consequently an increase of the etressea to 50-55 kg/mz
1/2
144-
USSR
GOL'TSMN, B. M. and KOMSSARCHIK, M. G., Fizika Tvardogo Tela, Vol 15,
No It Jan 73t PP 301-303
Measurement of conductance and the thermo-emf coefficiont in the films under
vaxious stress conditions indicates that the stresses acting in (Bisb)2Te films
3
Should essentially affect the electrical properties of the film. I figure
references.
2A
USSR UDC
GLASHICI Ili G. 41, Sen Lor ITI-t; Cri I C'toi- of tw III i-~ar 0y T;1,
Transportation Z" !'T"' Of Cilia 1'~i'v
Lahovatc.-.
d T r a r, s-, 1-) r 1: a to r. En -i,.% z,
Branch of the Khar'kov hi~s-titute of "ailro-
"Microelectronics in 'Railroad Automation and R(-r.-Mte (ctiitrc-I Sl---t
L
MOSCM7, AvLoviatilka. No It.) 1~71, -p 7-H)
Abstract: A StUd-7 of the po,,;sibility ot' usibij- od,:-rn micn)vloczrai-.4
media ill monitoring and control. systerar, for railroad tr.1i-IISnc---r---aLiO-.1, I'n
particular, centralizati-o-n. of dispatch control, the
and autortatic control.
Argt=ci-ts are for tiW
En'cr-lish and c---.:1L!ricnce i5 cited. The dj.a[-'Tn;'I5 C';
microcircuitr~ are discussed, azid it is ccnicludal C-lZat t- 1,:, (:%f lnLc~-
rrated circuits ill railro-ad autonation and ri~notc contrcl s)-;Lcr:7 lead Lo
conf;truction and installation
a decrease in t' I- -
quality relia'oility' a (Iccrease ill intake, hi';011 4'11LZICJS ci` Liz-
ntuaber of rCsPollse-S a decrease. ill the 10'-~d Of t1w -I :; i':! n I
cant raduction ill thc size of the LisLailations, e.'~cl LIS-` c'~I of
112
USS111
S 11:NKOV, G. A., et al., A-vtonatika. Telcmoklmni'ka i
GLASHCH
pp 7-10
systems and sclection of Parts, itISUrZ1,LLCC- of vibrat-iort aad
and resistance to corrosion, dia creation of standard units providin.-, ~for rc-
pairs at the ii,,odulc replacemenc level and ccanomically expwd-AienL reliainic
~duplication of the nucmuatic devices.
2/2
I ni 018 UNCL ASS I Hit)' PROCESSING DATE--13N0V70
DENSITY OIL WELL CEMENTS CONTAINING POWOERED COAL -U-
".--'AUTH0R-(0Z)-B EREZHNOY A. I K0444ck~~K S.S.
.' --COUNTRY OF INFO--USSR
,~_:SOUACE-NEFT. GAZOV. PROM. 970, Mv 24"5
~.D AT EPUBLIShED ------- 70
.,--SUBJECT AREAS--MATERIALS
-TOPIC TAGS--CEMENT, CG-ALt CALCIUM CHLORIDE, CHEMICAL REACTION RATE,
HARDNESS
C CNTROL MARKING--NO RESTRICTIONS
DOCUMENT CL ASS--UNCLASSIFfED
--:PROXY REEL/FAAME--3005/1969 STEP NO--UR/05131*10/000/001/0()2,4/0025
_.__CI_RC__.AC_CESSf_QN P40--AP013-3-813
.212 018 UNCL ASS IF I ED PROCESSLING DATE-- I-2NOV70
CIRC ACCESSION NO--AP01338i3
'ABSTqACT/EXTRACT--(U) GP-0- ABSTRACTo AN OIL WELL CEMEhl' wITH LOW 0.
(1.02-.1,5) IS -MADE BY INCORPORATING 33-66VERCENT POW0. CUAL IN CE.MENT
CON.TG..CACL SUBZ OR OTHER SALTS TO COiNTROL THF SETTING T[ME. UP TO
25PERCENr AIR 15 ENTRAINED WHEN THE COMPONENTS ARE MIXI'D. "I I TH
THE D. :Trll,)G TIME IS
INCREA,SING-COAL CONTENTP IS DECKEASED AND TH E S, 1.
-INCREASED.
UNCLASSIFIED
USSR UDC: 621.385
PIPKO A. I., GAVRILOV, A. A., %MI Sa -H.
"An Installation for Vacuum Treatment of the Cathode Elements of Magnetrons"
Moscow, Otkrytiya, Izobreteniya, Promyshlennyye Obrazt9y, Tovarnyye Znaki,
No 243 1970, Soviet Patent No 277119, Clas�.21, filed 2TDec 67, p (53
Abstract: This Author's Certificate introduces a device for vacuum treating
the-cathode elements of magnetrons. The unit contains a vorking chiuiber, a
prevacuum chamber, a loading box, and a table for holding parts with vacuum
electrical leads whieb can be moved out of the loading chamber into the work-
ing chamber. As a distinguishing feature cf the patent, provision is made
for checking the thermionic and secendary emission properties of the cathode
by equipping the installation with a measuring device mo,tnted on the working
m table. This device is made in the form of a cylindrical~anode with an
annulus in the middle, and an annular tungsten cathode siarrounding the anode
at the level of the annulus. The anode and cathode are fastened to insu-
lators, and the the inner surface of the anode acts as a collector of
secondary and reflected electrons from the cathodes bein$ inspected.
4 '4
USSR
and KMNMOV, V. G.
"Electron Microscope Investigation of Nerve Cells arA Their 10 hanges in
Hypotonic Sol-utions by the Sighting Nethod Used for the Study of Single
Cells pp 19-28, Sintez Belka i. Rezistentnost', Kletok, (Protein Synthesis
and Cell Resistance), Leeningrad, "Naukap" 1971, 104 pp,:
AbstTacts A study was made of the ultrastructure of pa=sympathetic neirre
cells in a frog auricle preparation (Rana, tesporaria) and their reaction to
damage by distilled i-rater. The article gives a description of the procedure
which nakes a sighting study of individual cells possible under both electron
and light microscopes.
M. W~l TMIL.7. r' 71 T: M- ........
USSR uDe: 621.373-52:621-373.42
KOHISS Asjj., ROZHANKOVSKIY, R. V.
"Investigation of a Sinusoidal Oscillator Based on a Circuit With Distrib-
uted RC Parameters"
Otbor i p--redacha inform. Resp. mezhved. sb. (Selectian and Transrdission of
Information. Republic Interdepartmental Collection), 1970, vyp. 25, pp
103-107 (from RZh-Radiotekhnika, No 1, Jan 71, Abstract No ID330)
Translation: The authors study harmonic distortions of the signals from, a
generator consisting of an emitter follaver and a distributed EC circuit
as a feedback link. Distributed circuits are analyzed, wid -u study is made
of the effect of circuit parameters on the shape of the emitted oscillations.
Bibliography of three titles, llesuA.
UNCLASStF
1/2 017 IEd
PROCESSING DAT_::-~--13NOV70
_TlTLfi--EFFECT OF CITRIC ACIO UN THE RESYNTHESIS A 0IN IN E
OF RAGbIl MU~CLE
14UCLEOT-IOES -U-
AI)THOR-(02)-KG,'41SSt.RE-i~IKOv S.V., PKHAKADZE G.A.
COUNTRY OF INFO--USSR
SOURCE--DOPOV. AKAD. NAUK UDR. RSRv SER. B 1970t 321,2), 171-3
DATE PUBLISHED ------- 70
SUBJECT AREAS--BIOLOGICAL ANO MED I CAL SCIENCES
JOPIC TAGS--RABBITf.P!USCLE PHYSIOLOGY, HEART MUS CLE, ADENOSINE
TRIPHJSPHATE
MAqKING--i"4O RESTRICTIONS
-DOCUIMENT CLASS--UNCLASSIFIEG
.-PROXY REEL/FRAME-3005/1~65 STEP ND--(JR/0442/70/032/002/Olti/0173
CIRC. ACCESSION iNO--AT0133570
E-D-
PRdCESSING DATE--13NOV70
212 ~Oi7 UNCLASSIFIED
`.,CIRC ACCESSICN NO--AT0133570
--A I.V. INJECTION OF CITRIC ACIO (10
T/ EXTRACT- (U) (;P-0- ABSTRACT.
MU, G-G.) ( I )DID %4J.T CHANGE A06NINE NUCLECTIDES CONfENT Iii KAW31T HEAAT
AND SK"LETAL MUSCLES BUT INCREASED INCCkP0kATI0N 13F GLYCINErliC PPIME14
INTO AOP OF SKELETAL, ANO ATPt A0Pj AND AMP OF HEAR T fo!USGLF IN VITRO I
ADIOACTIVITY :OF ADENINE
(4 lU -MOLES) INCIEASED SP. R %QCLEOTIOES, OF
DIAPHRAGM MUSCLE. FACILITY: I INS T .5 1 UKH 111. KIEVo USSRa
UNCLASSIFIED
Acc. X--: R. e -4
AP00523361
SOURCE: Fi~ziolo,'_Jchniy Zhurnal, 1970, Vol 16, Nri
PP 10
EFFECT OF o, p-DDD ON TRANSCORTIN-BINDING ABILITY IN DOGS
V. P. Komi sarenko, 0. S~ Alikosha, t4. D. Troniko
Department o Patophysiology, Institute of Endocrhotogy and Melabolism, Mea
Summary
Hydrocortisone content and the level. of, transcortin in plasnia of dogs were deter-
mined before and after o, p'-DDD administration.
It is noted that due to o, p-DDD administration a complete inKibition of 11-oxycor-
ficosteroid synthesis takes place.
Injecticns cf a, p'-DDD raised the transcortAn level. The. application of the inhibl-
tor did not change the protein concentration in plasma.
19820922
UNCLASSIF1 EC
-IT ITLE-STATE AN-r, FRCSPECTS IN THE OEVELOFM F
ENDCCP-I,KCLCGY;,.IN THE UKRAINE -U--
.,ltCEUNTRY'tF l,hFCr-USSR
:'4ClURCE-.FIZlCLCl;ICMY ZHURNAL9 1970v VCL 161 NR
!_,-~DA7E PUBLISHEC -,7C
PRCCESSING OATE-L7JUL70
BASIC PROBLEMS OF
?,v PP 19T-204
I;USJECT~AREAS-BIOLCGICAL AND MEDICAL SCIENCES
~.TIGPIC. TAGS-ENDOCRIhCLCGYp SECRETICNP CENTRAL NERVOUS SYSTEM* HORMONE*
STEP NC-UR/0238/70/016/002/0197/C204
IRC ACCESSICK NC--AP0052332
UNCLASSIFIEC
M
AF662332'- -77
so,."
PRINMIRY L.~,OE: Fiziolo-icliniy ZIL,.urna'JI-, MO, Vol 16, Nr
P P
STATE AND PROSPECTS IN T"E:DEVELOPMIENT OF BASIC
PROBLEMS OF ENDOCRINOLOGY IN THE. UKRAINE
V. P. ~ I(o rn 14 irenko
Institute Eadwittolo
g~~and MeMbolism, Kiev
Summary
The article deals with some basic achievements in the investigation of internal
secretion glands and the main trends in the studying such problems of endocrinology as:
1) 'interconnection of the central nervous system and hypothalamus in the regraiation
of endocrinous functions; 2) interrelation between the Internal secretion glands; 3)'rne;
chanism -of hormone effect. Great attention in the itrticle, is paid to the role of inhibitors
of the function of endo-crinous gland3 and their importance for clinical and experimental
endocrinology.
REEI~/Mlluk%fz
19820918
112 ozo UNCLASSIFIED
-,.TITLE-EMPLOYMENT OF INHIBITORS FOR REGULATION
-TREATMENT OF HERMONE CEPENDING TUMOURS -U--
AUTHOR-KOMISSAikENKOv V.P.
5UNTRY 'OF- INFG-USSR
-Cr
..SOURCE-VRACHEENOYE DELO, L9709 Nk 4t PP 13-18
,,,~:!DATE PUBLISHED----70
AREAS-BIOLOGICAL AND MEDICAL SCIENCES
TAGS-AGRENAL-CORTEX, BENZENE DERIVATIVEs
TUMOR* INHIBITION*.CHEMOTHERAPY
PROCESSING DATE--30OCT70
OF ENDOCRINE FUNCTIONS AND
CHLORINATED ORGANIC
-1-.4T~XGNTROL MARKING-NO RESTRICTIONS
~,-DQCUMENT CLASS-UNCLASSIFIED
..-'PROXY.REEL/FRAME--3001/1867 STEP NG-UR/0-ft75/TDIOOO/004,/0013/0018
;,~GtRC
ACCESSICN NO-AP0127277
UNCLASSIFIED
2/2 020 UNCLASSIFISD PROCESS ING DATE--30OCT70
CIRC ACCESSION NQ--AP0127Z77
ABSTRACT/EXTRACT--(U) GP-0- ABSTRACT. THE AUTHOR PRESENTS LITERARY DATA
ON ENDOCRINE FUNCTION INHIBITORS AND RESULTS OF STUDIED CARRIED OUT IN
THE KIEV SCIENTIFIC RESEARCH INSTITUTE 0,*r; ENDOCRINOLOGY 4ND METABOLISM
AND THE EFFECT OF DICHLGRUIPHENYLDICHLORETHA;IJE ON THE ADRENAL CORTEX IN
EXPERIMENTAL AND CLINICAL- CONDTIONS. RESULTS SUGGEST THAT
DICHLORDIPHENYLDICHLGRETHANE EXERTS AN EFFICIENT ACTION ON THE STRUCTURE
AND FUNCTION Of THE ADRENAL CORTEX %%HXCH OPENS PROSPECTS OF NEW
APPRAOCHES TO CHEMOTHERAPY OF HORMONE DEPENDENT TUMORS AND TREATMENT OF
1TSENKO CUSHING'S DISEASE.7 -FACILITY: AN VKR. SSR.
1/2 -017 UNCLASSIFIE:D PNOCESSIN" DATE-131NOV70
.TJ-TLE--THE IMPORTANCE CF DYSFUNCTION CF' THE AJKENALS IN THE PATHJGENESIS
MELLITUS ANU DIABETIC ANG110PATHIAS -U-.
"AU,THFJ,O,-(05)-KO.'IISSAPENKOt V.P.t YEFIMOVi~ A.S., POVOLUTSKAYA, G.m.,
LIMANSKAYA,""C.F., BEZVERKHAYA, T.P.
COUNTRY OF INFO--USSR
S.OURCE---KLlJNjICHESKAYA MEDITSINA, 1970t VOL 48 1 NR 5r~ PP
-0ATE PUBLISHED ------- 70
~~SUSJECT AREAS--BIOLOGICAL AND MEDICAL SCIENCES
JOPIC TAGS--ULABETES MELLITUSt ADRENAL GLAINDr HORMONE,
CaITROL AARKING--NO RESrRICTIONS
CLASS--UNCLA'SIFIED
-,:PROXY REEL/FRAME--3002/1772 STEP NU--UR/01,F97/70/C'48/.005/01181OL23
CIRC-ACCESSION NO--AP0129140.
Ul 14C. L A.S S II F 1)
mol
-7
-77777
~77.
2 017 UNCLASSIFIEO~ PROCESSING DATE-13NOV70
~~CIRC ACCESSION NQ--AP0129140
.~AgSTRACT/EXTRACT--(U) GP-0- ABSTRAC'r. THE COMPLEX EKAIM14ATIJ14 uF 151t
-.PATIENTS SUFFERING FROM OIABETES MELLITUS F.EVEALE13 lJYSFL;NCTIG"'j OF THE
ADREiNiLS MANIFESTEO BY AN JNCREAS~ OF THE GLUCOCORTFI-ili), ANDROGENIC AND
NAL FUNCTION I I -, R - UR T IGO I D
,ADRE, IN A SlAULIANEGUS REDUCTION OF THE~ ',INL ALCJG
ACTIVITY. THE NOTED D!STURBANCE WAS CHARACTERITIC: r-l-;R PATIENTS DURUNG,
DEMMIPENSATION OF THE DISEASE. WITH THE CONCOMITANICF- OF VASCULAR
-COMPLICATIOINS THERE. WAS SEEIN A I'QiE MARKEU RISE OF THE CATEClifjLA'lll%E AND
r4 ;r 11 S
AOROGEINIC ..ACTIVITY. GLUCJC0PN-flCOf0 HYPERFUNCTION ot. r E N L A
MORE PECULIAR TO PATIENTS -WITH plITIAL FUt"IC-TiONAL LEsljr,fS OF THE
VESSELS, A SUPPOSITIC'N' IS MADE JA THE POSSIBLE PATHCGEINETIC ROLF OF
HYP ER PRODUCT ION OF CONTKINSULAR AUr"ENAL HORMONES IN THE. GEVELUPMENT OF
FACILITY:, KIEV. N-1 lNSTITUT
-DIABETIC: ANGIOPATHfASo
:t'..~_:-,,EN0OKRI,%0LOGIl I 06MENA VESCHESTV.4
ljiq( L AS S I F I i:: 0
U 3
I l
- A
o
Zt It
or m lb
.
I
D
-" -
IS,
Ely
.
_
j
70
gay
LA
l-V
to a
F3 -
~_112 (339 UNCLASSIFIE kilICESSiING OA`TE-~-13.401170
-.`171TLE-CURR~~.ti`T OSCILLATIOINS IN BETA CANOTENE FILMS -u-
AUTH0R-(03)-SHJM0Vv YU.S., 'AIKHEYEVA, G.P., KOMISSARCI-V, &.G.
-COUNTRY OF INFn---USSR
SOU qCE-)fjKL. AKAO. NALJ.~ SSSR 19-10t 191(1)t 70-Z
--AjATE PUPL ISHEG -------70
-~-SVBJECT AREAS--PHYSICS, MATERIALS
JOPIC TA6S--SURFACE FIM CURRENT DENSITY, VO LT AMPERl-, CHARACTERISTICt
'T
01RECT CURREN LI'liT PIJL.SEt IMPURITY LEVEL, OSCIL-Livrion, oiGmF
Blu"CHEXISTRYt HYDROCARBON
,'-CONTROL MARKING--NO RESTRICTIONS
.00CE)MENT CLAS')--UNCLA'~'oSfFlEj'J
:PROXY RELL/FAAME-30031/1483 S T c" fN OUR 0 0 2 0019 1 /0,1-) 10 0 7 0o 0 7 2
_CTRC ACCE'SSIGN NO--AT0130412
IJW, L A S S I F I E 0
~/z 039 UNCLASSiFIED: PROCESSiNG DATE--13NOV7C
-IRC ACCESSION Nt3--AT0130412
:ABSTRACT/EXTRACT--(U) GP-0- ABSTRACT. SURFACE TYPE CELLS 1~c-:.'(E USED TO
+OLLOW- CURREW VAR I 4T [;:)NS IN ARWHOUS FILMS OF CA,"'ITENE AND ITS NIXTS.
WITH PROTOPORPHYRIN (1), JSING A TYPICAL Do C. SOUQ* CE WITH INTERMITrENT
TO LIGHT. TliE RESULTING CURRENT VOLTAGE (3-V) CURVES ARE
~Swlwr-l. CURREfg OSCILLATION'S ldlEkE 0850.~ONLY IN THE~FILMS THAT HAD BEEN
IGT C,'.110ENS AT I ON
FORMED aY FLO~WJG AND !,-l IN THE FILMS FORMED BY EVAPN.
THE I-V CHARACTERISTICS OF THE FILMS SO~PREPD. FRUM. THE MIXED PIGMENT
HAD OHMIC BEHAVIOR AT LOW FIEWS; AS THC FIELD WAS RAISED TO SATN. iv4OER
~BOTH DARK AND LIGHT CONDITIONSt THE CURRENT OSCILLATIONS 6--:GAN, AND THE
VALUE OF THkESHOLD P- 0. IN LIGHT NECESSARY FOR SUC0i 0SCILLAYIONS ~,As
SMALLER THAN THAT IN THE OAkK. AS THE CONCN. OF 1, INCRt ~:Dl THIS
THRESHOLD P- Do DECLUNED. THUS, THE I-APURITY INCRE-r-SED.THE POPULAT[ON
OF MICROHErEPOGEN IT LES IN THE VOL. OF 'THE PIGMENT Ali WELL ~S 1"4 -THE IONE
OF C9114TACT WITH THE ELECTRJUES. FACILITY: 14ST. KiilM. FIL.p
MOSCOW 'USSR
liNI'l L A S S I F I E 0
USSR UDC 615.31:547.718.11.012.1
KOCHERGIN, P. M., ULQS.SAROV I TKACHENKO, A. A., and VLASOV, V. V.,
All Union Scientific tijarmaceutical Research Institute imeni S.
Ordzhonikidze, Moscow, Zaporozhe Medical Institute, Donets Medical Institute
"Studies in the Imidazole Series. LII. Synthesis ana Pharmacological
Properties of the Derivatives of Imidazolino(1,2-f)xanthene"
Moscow, Khimiko-Farmatsevticheskiy Zhurnal, Vol 4s No 12, Dec 70, pp 14-18
Abstract: Starting from 8-bromo-, 8-amino-, and 8-methylmercaptotheophyllines
a series of imidozolino(1,2-f)xanthene derivatives was synthesized. Tneir
pharmacological action was investigated. The products exhibited a positive
inotropic action on frog's hNirt, comparable to that of theaphylline; they
lowered.the blood pressure and affected directly smooth:vascular muscles.
They shortened the latent period of conditional reflexes slowing down their
extinction; they increased the 'spontaneous' motor activity, but counteracted
the stimulating effect of theophylline on the motor activity of animals.
The compounds showed no 4ffect on the convulsive activity of corasol, hexenal,
or chloral hydrate. Several among them stimulated breathingt but were not
capable of counteracting the breathing inhibitory action. of morphine or hexenal.
USSR UDC 632.954
All
YATS M20 V. G. -Union Scientific Research
Institute of Sugar Beets
"Infiltration and Inactivation in the Soil of Herbicides Applied by
the Strip Method"
Moscow, Khimiya vSellskom Khozyaystve, Vol 8, No 9 (83), Sep 70,
pp 48-49
Abstract: Infiltration and inactivation of eptatm, sodium trichloro-
acetate and dichloralurea were studied after application of the herbi-
cides in strips 18-20 cm wide. Continuous application was also
used for comparison. It was found that eptam is absorbed by the soil
and therefore migrates only slightly with respect to the soil profile.
CZ)
Sodium trichloroacetate is washed out of the upper layers of the
boil into the lower layers, which explains its wreak effect on weeds
in years with heavy rainfall. Dichloralurea does not migrate through
the soil to any great exteat and is retained chiofly in the.upper
layer.
1/1
AdsorbtioA
USSR UDC 546.633:543-544.6
SHATSKIY, V. 14.,, KRMNK0, S. V., K0jYJZ$=VAr~~L*_jL., BEBMI G. F.
PHMOVA, X. M., KESIER, YA. A., and WOROGOV, V. A., Chain of Inorganic
Chemistry
"Synthesis of Novel Phosphorus Containing Sorbents and the Study of the Sorption
of Scandium on Them"
Moscow, Vestnik Pbskovskogo Universiteta, Vol 13, no 6, Nov-Dee 72, pp 653-655
Abstract: Optimal conditions for scandium sorption and separation from iron
have been determined on a pilot-plant scale. A specific sorbent was used in the
process. It was the product of the copolymerization of styrene with divinyl-
benzene phosphor~ylated with PNC1,;, and subsequently hydrolyzed with alcoholic
potassium hydroxide solution. Tlie opt:Lmal conditions fox, the separation process
on this sorbent are as follows: the sorption is carried out from a 0.1 11 Re 504
solution; a 7% ammonium fluoride solution is used for the desorption; under
these conditions in one "sorption-desorption" cycle the iron ir, isolated prac-
tically completely. Repetition of the desorption process trith a fresh portion
of the desorbent removed cQ% of scandium. Tais sorbent irmy be used for the con-
centration of scandium, out of the solutions-with hiGh iron content. Tn addition
to iron this method also separates all mono- and divalent elerrentB, rare earth
elements and other impurities from scandium.
412 010 UNCLASSI F.IEDI PROCE~SING DATE--I
3NOV70
TITLE-OETERMINATION OF GAS 1401STUREE -U-i-',
YU. A. KOMI SSAROVo N.14's BAKuLIN, A.,l-# OXHIGINY
VeS, kUlAVINt YE.I.
c cui-. R yoF two-ussR
26Lt740
3~.:-~tIEFE-'~E.NC~-:--&TKRYfLYAr 1LOBRET., P R 0,14. i~BRAZTSYt TOVARNY_
0,A r EPUBLISHED--13JAN70
'SUBjECT-A:.cAS- METHOOS AND E~WIPMENTo MATERIALS
TOPIC TAGS--SPECTROSCOPIC ANALYSIS# MOISTURE MEASUREMENT,
_GAS ANALYSIS.
-.CG,4TR0L,J4A9.XING--N0 RESTRICTIONS
,m~DOCUAENT CLASS--UNCLASSIFIED
~:~?ROXY REEL/FRAME--3005/0878 STEP
.-C. IRC ACC~5510N Nt)--AA0132968
UiNCLASS IF-IED
ZNAKI 19701 74(5)
CHEMICAL PATENTs
NO--Uft/0482/70/000/000/0000/0000
USSR uDc: 6,,j-525:621-375
tZSR Author's Certificate 14o 2542-08, filed 29 Jun 68, publishea 4 Mar 70
(from RZh-Av-,.c=ati'---a, Teier:12khaM-a, i _Vvchislitellmya Tekhnilm, -.o 11,
Yov 70, Abstract No IIIA3.02 P)
Translaticn: r7his Author's Certificate introduces a mf---u -ti r- ur
- =1 C P CS0, e
amlifier vith hig;:, precision. T'he wnplifier contains a conic,-t.L damper
Suspended bet-wreen hf&h-pressure eand low-pressu--- flows. -.he ccnica.1
of the &-t-mer ell,-~.zs its -~csitirin to be centered in the fjiw, and the vortex
1 ov whi ch develons at acertain value of the con-trolling -res5jure causes
the darmer to rotate, thus stabi ing its position. One ~Ilustra--ior-
T. R;
-1/2 034 UNCLASSI PIED PROCESSING DATE--230CT70
T-ITLE--REACTION OF BUTADIENE NITRILE RUBBERS WITH PHENOLFOR-NiALDEHYDE
ESINS IN THE PRESENCE OF HEXA14ETHYLENETETRAMINE -U-
P
':~,4UTHOR-(04)-OINZBURG, B.N.v CHECHIK9 L.E., KORISSAROV, S.A., BARAMBOYMt
N,. K .
-~t_CIU'l --USSR
NTRY OF INFO
,~..SOURCE-KAUCH. REZINA 1970# 29(2)t 10-12
DATE PUBLISHED ------- 70
'.,-.SUBJECT AREAS-MATERIALS
JOPIC TAGS--BUTAOtENE, NITRILE RUBBER* PHENOL FORMALOEHY0E RESINt
HEXAMETHYLENETETRAMINE, IR SPECTRUM# COPOLYMERs VULCANI LATE- t PLAST IC
MOLECULAR STRUCTUREt SPEC TROME TER/ (U) SKN40 NITRILE RUBBER11
:(U)NOVOLAK PHENOLIC RESIN, IU)URIO SPECTROMOTERv (U)UKC14- SPECTROSIETER
~'_.CONTROL MARKING--NO RESTRICTIONS
-,DOCUMENT CLASS--UNCLASSIFIED
PROXY REEL/FRAME--1997/0461 STEP NO-,-UR/0138/70/029/0i)2/0010/0012
CIRC ACCESSION NO--AP0119397
-212 034 UNCLASS I FIED PROCESSING DATE-230CTTC
CIRC ACCESSION NO--AP0119397
ABSTRACT/EXTIZACT--(LI) GP-0- ABSTRACT. THE REACTION OF SKN-40 RUBBER (1)
,.WITH A PHENCL CH SU62 0 NOVOLAK RESIN L8 (II)o HEXAMErHYLENETETRAMINE
_(lIl)r AND S WAS STUDIED BY IR SPECTROSCOPY. MODEL I-If-H[ MIXTS. WERE
MILLED AT 30-40DEGREES AND MOLDED AT 155DEGReCS FOq 20 HR, AND THE
PRODUCTS WERE EXAMO. IN UR-10 AND UKC-14 SPECTROMETERS OVFR A WIDE RANGE
OF FREQUENCIES. I AND 11 REACTED DURING MILLING TO GIVE R-11 COPOLYMERS
.(THE AMT. OF COPOLYMERS FORMED DEPENDS ON THE 1-11 RATIO AND PROCESSING
CONDITIONS 1. MOLDING AND HEAT TREATMEINT OF I COMPNS, WAS ACCOM13ANIED BY
HARDENING OF II WITH III, A REACTION BETWEEN lo Ilt AND Illp AS WELL AS
A REACTION BETWEEN St ly AND 11- THE REACTION LED TO THE FORMATIOU OF
SUPRAMOL. STRUCTURES WHICH IMPROVED THE PHYSICOMECH. PROPERTIES OF THE
VULCANIZATESs FACILITY: VSES. NAUCH.-ISSLED. INST. PLE?,lOC.HNYKH,
--,~-.MAT.ER. ISKUSSTV. KOZHIr MOSCOW, USSR.
ICLAS-SIFLEG
101706b Effect of the extent of orientation on the kinetics of
(
the mechanical degradation of ?9lymers. Ko I 7v, Sti A
mv, I I.- B
Aleksan WSCOOZ51"C ~
aramboirn,
orn.. Nfoasu"OW, V~'*K . I'A-.~
'101, Snedin., B 1971).
12(2), 112-14 (Ru E.). The. method 61 Imst squares was usM to
derive an eq,iation describing th6 inkh. degradation of Kaproji,
Lavsan, and Nitron fibers takiz e a ru
_kg-inio ii~count th ' t ctural ot-
dering coaffs, An ii~untii~n. relatiog the. elonfation Multiplicity
factor, the mot. wt., and th di t me or highly orienttd
e ispersion
systems was also denved. Thp ~ equation; Af r tu (Mo
M. 182 6 + 6750,' where M7- '- mot. %1.. at any
time r, Mo - initial mot. wt., M.:- limiting mot. wt.. and :r
the elongation multiplicity factor, satisfactorily desicribea-I the
mech. degradation of Nitron. fibers. DBJR J
REEL/FRAME 7
l 12 016 UNCLASSIFIED PROCESSING DATE--30OCT70
_~-TITLE_KINETICS AND MECHANISM OF METHYL ETHYL KETONE OKIDATIUN IN THE
R* - Lt-
ESENC,E OF COMPLE,XES OF IRONvIllt AND 9olPHENANTHROLINE
WHOR-102I.KUMISSAR D., DENISOVo YE.T.
~'--CCUNTAY OF INFn--;-USSR
bbit 1970, 44 (2) 390-5
ZH..FIZ. KHIM.
BLISHED-70
SUBJECT AREAS-CHEMISTRY
PIC TAGS-CHEMICAL KINETICSt METHYL ETHYL KETONE9 CATALYTIC OXIDATION,
,,,.,,-CHEMICAL REACTION MECHANISMv IRON COMPOUNUP COMPLEX COMPOUND, CATALYST
REGENERATION
..CCNTROL MARKING-NO RESTRICTIONS
DOCUMENT CLASS-UNCLASSIFIED
REEL/FRAME--2000/0891 STEP NO--UR/0076/70/044/002/0390/0395
CIRC ACCESSION NO--AP01245S4
2/2- 016 UNCLASSIFIED PROCESSING OATE-3oacy7o
.,ClRc. ACCESSICN NO-AP0124554
.,,,,:ABSTRACT/EXTRACT-(U) GP-0- ABSTRACT. KINETIC DATA ON THE OXION. OF ACET
-SOLN. BY MOL. 0 CATALYZED BY FE(II11,09PHENANTHROLINE COMPLEXES
IN,AQ.
Ir
(1) INDICATE THAT THE MECHANISM INVOLVES OXION. OF MECH:C(DHIME BY 1 0
.,.MEC:C(OTIPES)NE, WHICH DECOMP. TO MECH TIMES AC* WHICH HE-ACTS WITH 0 TO
FORM MECH(OOH)ACt WHICH UECOMPo BOTH TO FREE RADICALS THAT ACCELERATE
~THE OXION. NAD TO THE UXLDN* PRODUCTS ACH AND ACOH. THE OVERALL RATE
DEPENDS GN PH AND 0 PRESSURE. THE AMT. OF FE(III) THAT IS REDUCED
LEVELS OFF AT 60PERCENT DURING THE OXIDN.v INDICATING REGENREATIONo
FAC I L I TY: v CHERNOGOLOVKAv USSR4
FILIAL INST. KHIM. FIZ.
Heat reattieht
USSR mc.621.791.856.3:62o.193-41
YURCUOKO, YU. F., SCTNICHENKO, A. L., AZAPOV, G. I., KOIIU AROV, V. G., and
0-41
SHURAKOV, S. A. -
."Effect of Heat Treatment on the Sti-acture and Corrosion~Resistance of the
Metal In the Heat-Affected Zone of joints of ?1~28NIOT Str_-el"
Kiev, Avtomaticheskaya Svarka, No 6. Jun 71, PP 8-11
Abstract: Studies were made on joints of lEhl8NlOT pipe 57 mm in dianneter
with a wall thickness of 3 mm produced by argon-are welding. A-fter welding, a
portion of the joints were tempered Ft 7000C for 2,10, 1W, and 1000 hours:
the other portion was quenched in water after heating for different times at
1000-12500C. Heat treatment of lXhl8JI0T weld joints inc---easeA the rate of
knife corrosion and expands the front of its development. Thio, was caused by
precipitation, at this temperature, of chronium carbides (if the type Me2~CtS
along the grain boundaries of the hea7-affected zone. floldinr, tit WOOC 0~
10-100 hours leads to coalescence and disoolution of, zhese carbides and to
the appearance of the sigma-phase at the grain 'L %rien, in this case the
=nd,
carbon, being freed in the dizZo3ution of' meta.3tatble chrrj.,Alt~!n rn;rbid,~-2;, i,,;;
L --ically distribut,-2d In thc: br;dlr of
bonded in caebides of titanium vhic ~xe baa
4:3s divieiiinho!7, the rttt& or 4,nilf,~, ~-orra,,Ari-,-i.
nuatenite grains. How,.,vor thi;) procr~
froin 10W-115V-~C lx,,era (by 1.5-5 timen) ~b-- r! t f
Quenching Joints !,P I C
1/P
"'Til MITI I M
H.H."KH, IM
USSR
YURCHENNO, YU. F., etal, Kiev, Avtomatiche5kaya Svarka, No 6, Jun 71, P-P 8-11
corrosion. This has been associated with a change in the type of c&rbides of
titanium in the heat-affected zone, --y redistribution and removal of internal
stresses, as well as with the elimnination of concentratior, heterogeneity of
austenite in grain bodies and in their boundaries. increasing quenching
temperature (1150-12500C) leads to facmogenization of all zone,.: of the weld
joint and prevents knife corrosion; Reheating joints fo-r qtienching above 1250-3c
increases the rate of knife corrosion. 7 figures, 2 bibliographical references.
USSR
KLIGER, G.A., KOMISSAROY, V.I., KUZWETSOV, V.D.
nWide-Band Balancing Transformer (Short Report)
Elektroavyazl, No 9, Sept 1972, DP 17-19
UDO 621-372-855
Abstract: Previous works with V.D. Kuznetaov as a coauthor deocribed a number
or schemes for wide-band balancin'p- adapters with transformution, which are used
for accordant connections of eym-metrical and nonsymmetrioul lines v'ith various
wave impedances. Because it is di!ficult to make a symmetrical line with the low
wave impedance required, particularly in the short wave range, tle present p5per
presents a method for simplifying the design of rjuch a adLpter and de-
creasing its length by half. The raethod is based on a sch,~~rjie previouoly propoeed
by the authors (Author's Certificate No ~4~~27, "Byulleten', iz0breteniy," No '20,
1972). An analysis is made of the adapter in order to dertern-ine th~- optim.1-1 naz-
nitudes of the wave impedances WT and Ws- 7 fig. 4 ref. Re-celved by editors, 6
SePt 1971.
USSR UDG 621.3%.679j621072-5
KUZNITSGVt V.D.t KOMISS&O-V V014
aNoncontact T=ing Of Traveling-Wave Feeder"
Elektroevyazi, No 4, Apr 19721, PP 68-71
Abstreett A noncentact tuning eyetem is described which permita smooth fine
tuning of a traveling-wave feeder line for matching, withriut disconnecting the
transmitter and to eliminate in practice the possibility of an incorrect abrupt
miezatoh of the line. Formulas and curves are presented which make it p0aviblo
to produce a design of the device, and poesIble constructiva achemae of the
for a two-oonductor symmetricalifeeaor are diacuasod. The electricel
arrangement
Btability of the device in evaluated.~ 9 fig. Received by 4-ditors, 24 June 197L,
USSR uDc 547,565.2
PAUSHKIN, YA. M., LUNIN, A. F., and KOMI Moscow Institute
of Petrochemical and Gas Industry Imeii-r-1-.M. GUME
"Synthesis of Thermally Stable Oxidation-Reduction Polymers"
Moscow, Doklady Akademii Nauk SSSR, Vol 195, No.5, Dec 70, pp 1125-1127
Abstracts In light of the increasing interest in redox polymers, a
synthetic route was developed based an heterocondensation of disodium
acdtylenide (DNaAc) with 2,5-dibromoquinone (DBq) and 1,4-dimethoxy-
2,5-dibromobenzene followed by demethoxylation with HI, It was deter-
mined that the redox capacity of the polymer drops with Increased re-
action temperature, which may be due to partial brosalinking and de-
hydration. The polymer obtained maintained its redox capacity for
10 hrs even when heated in air to 3000C. This polymer shows semi-
conductive properties. The synthesis took place In two atagest first
stage was carried out in a flask in hexadecane modium, with reaction
temperature of 2500. The process lasted 10 hra in argon atmosphere.
The ratio of DNaAc to DBQ was 2sle Second stage was carried out In
solid phase In temperature range 300-4500 yieldb% the polymers, a black
powder insoluble in water or organic solventa.
ACC''O' NIr- Abstkactibg' 'SefVide: Ref.- Code:
AL ABST.0'
00052503 CHEMIC 0101"
101323z Synthesis and Propertim . of new aro~atle I
Mon. Paushkin; Ya. M Mkinsw
-4. nin A, e
Y-J.; Lu
sandrovZ-V. A.: Uganesov--T- S.,
Meshchiryakov. Y -
-m. IM. OL4-
mov. V. N. (Inst. Nift-eTg ~jmaa (;uhki-.1 o9
cow, USSU). -VYSOA-OM--01. zioecaulm,~ Ser. :B Mr(u, 12111P. 53-6
(Ituss). The beterapolyci~ndensation:of.NiiiC2 with and
p-CsKC12 and C-GH4Br2, 1,4-,C,JIEIrJ~ and 1,5-CaBsUrr, rmO
9,10-dibrornoanthracene in CjrHu *as studied under Ar at
.200-87*. The most reactive monomers were the o-dibroni6 deriva.
The polymers were brown to black powd6rs stable at up to SOO-400%
having an elec. cond. in the range of W-7-10-12 (ohm cm)'-'. The
polymers were readily nitrated, sulfonated, and aminaW. eg.,
suffonation with iurning If2SO4 gave beat -MiStant (to 300*) C114-
ion exchange resins I of high exchange capaci.ty. CXJR
REEL/FRAKE
+ ~&
19821144
USSR uDc: 6P-1-315-500
VOROB'YEV L. Ye. KOTT and STMEYEV V. I~, 1,eningrad Polytech-
nical Institute iw,-., -771 inin
"Double Beam Refraction With Hot Electrans In the Infrared Region in Degenerate
InAsit
Leningrad, Fizil a i tel-lunika zolaprovodnikov, vol 6, 110 6, 1972,
pp 1153-1155
Abstract: This brief communication is based on an earlier raper
by the three authors named above (Phys. St.'Sol., 50, 1972) In
(# 1-he dielectric permeabilitTl)ecomes an
which it was shown tha-- t
anisotropic quantity i_-1 strong electric fields aio, ~Jie result of
the anisotropy ol' the distribution function of hot, current car-
riers, and of the nonparabolicity of the conductive mone. The
arisotropy of the index- of refraction leads to a shi4L It in phnse
-for light polarized parallel and. perpendicular to t1an strong
field. in the TY."caent oaper, double rofractiorl io ii-..vUStj.,-atC-d
in n-type Irdis at a temperatun of 800 X. The carriev concen-
I 1b per cc, and the electronic gas is
tration in the InhS is 1.5-10
ireak-ly. degenerate. The experimental method is fully described -in
another earlier paper by these same authors ('Lietters, ZhE~2'2,
1971, p 140). Curves are plotted for the anisotropy of the in-
dex of refraction and for the electron temperature ar, functions
of the electric field intensity; good agreement between the raea-
sured and comDuted values is shoun.
USSR UDC: 531.715.2 531-717-53
SHATALOV, V. F. , KOPYTIIJI, A. M. , PONPRIN, N. S. , KOHISSAROV, V. T.
"A Method of Determining the Extent of a Destroyed Layer ~in Semiconductor
Plates"
Yoscov, Gtkntiya, Izobrete-riiy,~~,_ELoty.~Lb:~,a4nyye Ojjra~t '~o ig Znalki,
No 7, Mar 72, Author's Certificate No 329374, Division 0, filed 7 Apr 70,
Published 9 Feb 72, p 151
Translation: This Author's Certificate introduces a method of determining
the extent of a destroyed layer in semiconductor plates. 'The procedure
consists in etching the surface of the plate in wi electrolyte and measur-
ing the paraneters of plates. As a distinguishing feature of the patent,
the method is designed for increased inspection productivity. A strain
gauge is used for determining the greatest deformation of the -plate during
the etching process.
to
USSR UDC 621.396.677
MaSSAROV PAVLYbK, V. A., KRIVOSHEYEV, YE. F., OSTROVSKAYA, L. S.
"Experimental Study of a Diffraction Probleie'
Radiotekhnika. Resp. mezhved. nauchno-tekhn. sb. (Radio 1-ngineering. Republic
Interdepartmental Scientific and Technica1Collection), 1970, vyp. 14, pp 106-
109 (from RZh-Radiotekhnika. No 4. Apr 71,.Abstract No 031)
Translation: The diffraction properties of periodic antenna arrays are in-
vestigated. There are 3 illustrations and'a 3-entry bibliography.
A/Z 036 UNCLASSIFIED PROCESSING DATE--30OCT70
-T.ITLE--STABIL.ITY OF THE STEADY COMBUSTION REGIME or-A SOLID FUEL -U-
,~.AUTHOR-102)-KOMISSAROVAP G.101 SULIMA, U.10.
_~-.COUNTRY OF INFO--USSR
-:SOURCE-PMTF ZHURNAL PRIKLADNOI MEKHANIKI.I TEKHNICHESKOI FIZIKIr
.~.::~~JAN.-FEB. 1970, P. 163-167
PUdLISHED ------- 70-
SUBJECT AREAS--PROPULSION AND FUELS
_.--~,T'OPIC TAGS--SOLIO PROPELLANT COMBUSTIONP COMBUSTION STABILITYr COMBUSTION
,.ANAL YS I S
:'ZONTROL MAAKING--NO RESTRICTIONS
:,DOCUMENT CLASS--UNCLASSIFfEO
'PROXY REEL/FRAME--1996/1542 STEP NO--UR/0207/70/000/000/0163/0167
CIRC ACCESSION NO--AP0118525
UNC LASS I F I:E0
.......... ...... ...
7-._-',7_12 036 UNCLASSIFIED PROCESSING DATE--30OCT70
.CIRC ACCESSION NG--AP0118525
ABSTRACT/EXTRACT--(U) GP-0- ABSTRACT. STUDY OF THE EFFECT OF HEAT
GENERATION IN THE REACTION ZONES AND OF AN INHOMOGENEITY IN THE
TEMPERATURE AND VELOCITY FIELDS ON THE STABILITY OF THE STEADY
COMBUSTION REGIME OF A SOLID FUEL, USING THE METHOD OF SMALL
PERTURBATIONS, A NEW CRITERION OF STABILITY OF THE STEADY COMBUSTION
-REGIME OF A SOLIO FUEL IS OBTAINED, AND THE PARAMETERS ESSENTIALLY
AFFECTING THE STABILITY ARE DETERMINED. THE PROBLEM 15 SOLVED IN A ONE
DIMENSIONAL FORMULATION, ASSUMING THAT THE COORDINATE SYSTEM IS
INVARIABLY CONNECTED TO THE BOUNDARY SEPARATING THE DOLID FUEL FROM ITS
DECOMPOSITION PRODUCTS.
UD04- 533.9.082.5
IGNATCV, A. B., KOMISSAROVA, 1. 1., 03TROVSKAYIi, 0. V., and
SHAPIRO, L.
"Double-Wavelength,Sinl~,le-1,3xDosu-re Holographic Plasma Inter-
ferometry"
Leningrad, Zhurnal Tekhnichoskoy Fiziki, voi. 41, No. 2, 1971,
pp 417-423
Abstract: This paper is connected with an article written by the
third-napied of ihe authors above.and pqblished in the same jotirnal
(vol. 40, No. 11, 1970). In this earlier nrticle the a'utl~or' prop o sed
a method of double -wavel eng-U*,, singl e -exposure nolo,'"raphic interfere-
metry in vhich the form and pos Ition of the interfy.-r,_~nce bandS are
determined only by the dispersion characteristics of the investi-
gated object. Essentially, this method involves two wavelengths,
one of which is half the other, radiated by a hologram of a phased
object on photomat~arial with a light -uransmissivity i-.rhich is a non-
linear function of the illwii-nation on it, In the T)r~~sent papert
-1/2
USSIR
BNATOV, k. B., et al, Zhurml Takhrxicheskoy Fiziki, Vol, 41, No-_Z, 1971,
pp 41?-423
a closer and more detailed look is taken at this method, and a de-
scription is given of the first attempt to use it for in"V-erferomt_:t-
ric invest4LE;ation of a plasma. The atithors found 11-hat; dispersion
interferometry gives rE~sults which are inferior to those of tht.!ir
method. They are with the A. F. loffe Physico-Teehnical Institute
of Leningrad.
2/2
9(
USSR
to 620o.193.5
NIMINO V. I., KOMISSAROVA. 1. P., and PKNKRAT'YEVA, N. V., Academy of Civil
Aviationj Central scientific Researchg Planning and Design Institute Ineni
L 1. Polzunovt Leningrad
"Experimental Verification of the Parametric Methcd of Wculating the Heat
Resistance of Metals at Varying Temperature"
Kievi Fiziko-Khimicheskaya Melchanika Materialov, Vol 9,
No 5, 1973, PP 71-75
Abstract: steel brands 20t Khl8NlOT, and Kh25T were subjec-
ging tem-
ted to heat resistance tests in air under steplike, chang
perature conditions, the interval of the latter being up to 1500.
"I -
4-
A graphic variant of the parametric method basea on ,he use of
an equivalent time nomogram and the parametric heat resistance
diagram. were used for the calculation of the characteristic of
heat resistance, the mass loss of the metal. Tabulated experimen-
tal data of the mass loss of the first.two steel brands at two-
1/2
42 -
USSR
NIKITIN* V. I., at a1.$ Fiziko-Khimichaskaya Makhanika Materialov, Vol 9,
No 5t 1973# PP 71-75
-step and multistep tem-perature change are in good agreement
with calculated data (Maximttm difference 22% and 24%, respecti-
vely). The correlation of calculated and experimental data for
Kh25T steel shows a maximwm difference of 15% at relatively com-
plex multistep temperature change*conditi.ons. The investigations
indicate the possibility of calculating with sufficient accuracy
the heat re31stanne of metals at changing temberature by the pa-
rametric method. Three figures, three tables, three bibliographic
references.
2/2
USSIZ
UDC: 536.5:621.383
Anufriev, A. A., Komissarova. L-H., Sak)tarov,'V. P.
"Photoelectric Sensor for Recording of Low-power 1nfrared Radiation"
Moscow, Pribory i Sistemy Upravieniya, No 5, 1972, pp 4.8-49.
Abstract: The sensor described in this article was designed for recording weak
light signals radiated by heated substances in an adiabatic coinpression chwaber.
The sensor consists of an optical aperture, light guide, interference light
filter, modulator disc, photoresistor and standard signal source. The device
can record signals taken from the photaresistor in the range of 2-20 -Pv with a
time constant of about 10-3 see, with linear accelerations up to 150 g and
vibrations at 100-2000 liz, apd therefore can be used. for a niunber of Problems
where the properties of a gas and control *of a process in the gas involve the
radiaiton of light energy.
1/1
-4WW
USSR UDC 546,68263+546.824-31
ROWIN, 1. A., SPIRIDONOV, F. M11 QQPAJ11VA_ and PLYUSHCHov, V. YE.,
Moscow Institute of Fine Chemical Technology imenr7l, Y. Lomonosov
"Interaction of Titanium Dioxide With Indium Oxide"
Moscow, Izvestiya Akademii naulk SSSR, Noorganicheskiye auterialy, Vol 7,
Ho 10, Oct 71, pp 1798-1800
Abstract: Described here are j~efined conditions for the synthesis of Indium
titanate ag well as the nature of the interaction of In2 03with TiO2 . The
interaction was studied on specimens prepared by the simultaneous precipita-
tion of hydroxides from chloride and nitrate solutions of In and Ti salts
using ammonia. The x-ray diffraction study indicates that the reaction
product -- indium titanate -- exists in the narrow region near the 50%f
mol. wt. TiU2 and is of the formula In2TiO5 it is clused with the rhombic
aystem with parameters a0=10.47-, b0=9.895; co=14.51X. -In2TiO5is a white
substance; it raelts at 17500C. Relative to crystal optits, In;,TiO is
5
1/2
USSR
ROZDIN, I. A., et al, Izvestiya Akademii nauk SSSR, Neorganicheskiye
materialy, Vol 7, No 10, Oct Tl, pp 1798-1800
anisotropic vith an index of refraction >1.76. After having been fired for
3 hrs, In2TiO5 will not dissolve in 25% KNO3 but almost totally decomposes
in HCl (1:1) with In going into the solution and Ti remadning in the precip-
Itate. There are no amalogs for the In 203-TiO2 system in reference litera-
ture. (3 illustrations, 3 bibliographic references).
USSR UDC 546.681.3'824:542.915
SPIRIDONOV, F. M., ROZDIN, I. A., SO", IKOVA, M. N..p_KQAJj2a1~?VA, L. N., and
PLYUSHCHEV, V. Ye., Moscow State University imeni If. Vi Lomon0`s0_V'_,* Moscow
Institute of Fine Chemical Technology imeni M. V. Lomonosov
"Gallium Titanates"
Moscow, Izvestiya Akademii Nauk SSSR, Neorganicheskiye Materialy, Vol 7,
No 5, May 71, pp 817-824
Abstract: A detailed study of gallium titanates by the method of roent-
genographic analysis is presented. The experimental technique is briefly
described. Gallium metatitanates, dititanates, and titanates were con-
sidered, and experimental data presented :in tabular form show that the
first two are formed at 1400*C and the latter at 950%. The galliu-m me-
tatitanate is stable at more than 1100%, and in a metaptableu state it
undergoes a polymorphic transformation at- 960*. The dititanate is an
unstable compound having a series of polymorphic transformations. The
6-phase (having a deformed rutile lattice) is the most 4;table gallium
titanate. Melting points of gallium titanates are 1590 + 20*C fQr
Ga203-T' 03; 1680 + 500C for Ga203-2 Ti 02; and 1860 + ~OC for the
6-phase.
9 053075-
UR 0289
PRI'MARY SOURCE: Izvestiya Sibirskogo Otdelenfya, AZI S S S R
S
eriya nimichleskikh Nauk, Nr 12(162), Nr 5,
pp
n 11
N. P. A n 0 v h
V. M. S c'h 0 "1 xv,
1 T
ON THE SOLUBI'ITY SCAN DI MAI"M 'MMATES TYPE
MSc(Cr04)2 IN THE WATE[t SOLUTIONS M2CrO4 AND AI,Cr2O-.
The solubility AISc (CrOj): 2H20 (M=NH4, No, K)'; is stuilied in fl-ic solutior;s of
chromate and dichroinate of alkaly inetals and ammonium, correi;panditiry to them.
O-L
1/2 012 UNCL ASS I F It'D RAOCESSING DATE-13SEPTO
~~-TITLE-THERMAL STABILITY OF SCANDIUM HYDROXIDE TH!ncYANATE -IJ-
AUTHOR-(04)-GULIA,
V.G.# KOMISSAROVAf L *N.t KRASNOVARSKAYAt A.A., SAS,
14.
.1
T
,,::C-CUNTRY OF INFO--USSR
SOURCE--VESTN. MOSK. UNIV., KHIM. 197?,emn)
...A)ATE PUBLISHED ------- 70
*2'-SUBJECT ARF.AS--CHEMISTRY
...TOP[C TAGS--THERMAL STABILITY, SCANDIUM
..~:~HYOROLYSISt CHEMICAL DECOMPOSITION
CONTROL MARK (NG--.N?C RESTR ICT 10? S
-.:.0OCUmENT CLASS--UNCLASSIFIFD
REEL/FRAME--1987/1098 STEP
CIRC ACCESSION N0--AP0104496
UNC LA S S I F I E D
38-41
COMPOUNDi HYDROXIDE, TH113CYANATE,
2/2 012 UNCLASSIFIED PROCESSIN3 DATE-18SEP70
,,:CIRC ACCESSION NO--AP0104496
ABSTRACT/EXTRACT--(U) GP-0- ABSTRACT. THE THERMAL ST.49>1t.ury OF SC
HYDROXIDE THInCYANATE SC SUB4 (Oli)SUB?(NCS)SUB10.11H St),,52 0 IS STUDIED.
THE COMPD. IS COMPLETELY u.-qs'rABLC- IN Ala EV2N AT noom ump. IT IS
HYDROSCOPICt 48SORBS MOISTURE INCREASING ITS WT. OY 24,71PERI-eMT, AND
THEN SLOWLY DECOMPS. BY HYDROLYSIS.
it njz~ Set# :ce'.
Abstric i
tit
593 BST
CHEKCAL A (0 110
411f
'-117254p Properties of zirc~nlum and bdnJunVol"rop tes.
zprQvskjiXa. Z..X,;
(USSR)- Zh. Neorg. Khi?A.. 1970, 15(2), uss
Products of thermal decomon' of MO(EtCO:~~.160 (M i ,
Zror
HO were, at 5 '0-1300, * M6(EtCOj)t.0.5Hj0;~' at 1 bO-250
W203(EtIC02)1; andi atAO-W, hf0j; anal;~,ses are given.
Intermediate products-of the decomion. did not.wntain ihe M:O
-D* -of is6thernud ~Wj. of 'MO(Et-
groqp (ir spectral., . tngr2ws,
C00i-HiO in EtCO,,H were constructed and the ponipns'. of liq,
and solid phases are tabulated. . The conipn', of 'the solid phase
(MO(MM)t.140) in the 10-100 wt. go' pro~iqnic acid range
remained unchanged.
REEL/FRMfE
Acc Nr: Abstracting Service: Ref. Code:
A~005- 5938
CHEMICAL ABST. 70
11728he zirconiurn and baffiluni nitrobenzoates. S-nirnov
V. A.; Prozoro,6-kavti. Z. N.; ILljmii~
--M-95cow 1. SR ~. Z R', . Nerrg 1970, ~5(~2),
341 -CY (Russ~. of 7r or fff react
with p- or t-i-nitrubenoic aclid to give
Zr or Hi ; ur 140"': 6 and Iffift-C-114C),N4. Msp.
TfiL, compd- ikcrt~ studk-] by DTA an,--l thermoi-rav-.1metty. Zr-
t. at-.d &L,:jmj)- Ou-nnally to
Zr,O,(CII1jQ4N)c, -inti ZrO~, a;z(l
N f s Zri)(C-HAN' in w)(111. to the
Auah),*W~-!N MIQ1-0111404N arli'l
-11404 (C and 11R.), alid FIf,, I)-C-,l I.-
O,N 14 f'lrln'~ I ifL()(LC:11,04N 'r, in 4('11111. to tile nit-vtic"nud coinj "'lb.
Activa-t-un cur -na.
I gies of th~r~ decapirm. of I m.-re -20-1. kc-A!,
mole and of were 41 and 46 for
MI Zr ant! 11f, resi).
HAlp
REEL/ FWIE
LIZ GC9 UNCL4SSIFIED PROCESSING
TITLIE-CUMPUSITION ANU SCME PhOPERTIES OF COMPLEX SCA,NDIUM SULFATES -U-
:,AUTHOR-103)-SFAISKIY, V.M., KGMISSAROVA# L.114.9 BASHKOV, 8.1.
CEUNTRY CF INFG-USSR
CURCE-ZHO NEORG. KH[Mo 1970, 15(4)v 9 7 1~8
,'~DATE PUBLISHED------70
,:,:,sUt3JECT AREAS--CHEMISTRY
"-.TCP-IIC TAGS--CCIJPLEX COMPOUNU, SCANDIUM COMPLEX, SULFATE. THERMAL
.-.-,..:.DECLMPOSITICN
t&4TROL XAF.-KING-7410 RESTRICTIONS
CLASS--UNCLASSIFIED
REEL/FkAME--3002/1166 STEP NC--1)9/0073/7OiOl5/004/0978/0982
.-CIRC. ACCESSICN NC---AP0128588
2/2 0c'; UNCLASS I F I ED PROCESSING DATE---20NOV70
~~-CtRC ACCESSIGN NO--AP0128586
'-ABSTRACT/EXTRACT-W) GP-0- ABSTRACT. SULY, DIAGRAM OF (NH SU134) SUB2 SO
-SU84 NEGATIVE SC SU02 (50 SUB4) SU83 NEGATIVE H SU02 0 SYSTEM AT
25DEGREES IS PRESENTED. THE SYSTEM FORMS NH SUB4 S-C(SO SU64) SUB2 (1)
(NH SUb4) SUB3 SC(SO SU04) SU83 (11). Iv HAVING NS, ALPHA 1.560 PLUS
OR MINUS C.003 AND GAMMA 1.565 PLUS CR MINUS 0.1)03 IS Tlil'RMALLY STABLE
-TF -GREES
SMALLER AN OR EQUAL TO 390DEGREESt. DECOMP14. AT LARGER rHAN3900C
-E-Sw '10 SC SU62 0
TO S-el' SL182(SO SUBil SUi33 AND AT LARGER THAN d5U0EGRC-
SU83o T17ERMALLY LESS STA6LE 11 UECOMP. Al 330-405DEGREL-S TO I AND THEN
TO SL SUB21SO SUB4) SU63 AND FINALLY TU~SC. S682 6~ 5UB3.'
FACILITY.' MUSK, GUS. UNIV. IM. LUMCNOSUVA# MOSCCI%p USSR.
UNCLASSIFIED PROCESSING DATE--04DEC70
1/2 017
TITLE-THIOCYANATOSCANDATES OF SOME QUATERNAkY AMMUNIUpt BASES -U-
YU.G., KATOCHKINA, V.S., KOMISSARWIAt L.N*
OF INFO--USSR
:~-_SOURCE-ZH. NEORG. KHIM. 1970p 15(5)l 1248-54
PUBLISHED ------- 70
SUBJECT AREAS--CHEMISTRY
_~_"-TOPIC- TAGS-COMPLEX COMPOUND, THIOCYANATEt SCANDIU14 COMPOUND, QUARTERNARY
AM, ONIUM SALT, ELECTRIC CONDUCT IVl TYIJELECTROLY TEv THE MAL OECOMPOSITION
~,--;-`~'CONTROL MARKING--NO RESTRICTIONS
:DOCUMENT CLASS--UNCLASSIFIED
PROXY REEL./FRAME--3007/0740 STEP
CIRC ACCESSION NO--APoI3fjt79
-fill-
MUMIN'SIR MIR ".1 f HIMME vi
212 017 UNCLASSIFIED MOCESSENG DATE--04DEC70
CIRC ACCESSION NO--AP0136179
ABSTRACT/EXTRACT--(U) GP-0- ABSTRACT* SOLY, OF (R SUB,'~- ~4) SUB3 4SC(NCSI
SU86)-(Il (R EQUALS ME7 ET, OR BU) IN,H SUB2 0, MECOE*r, ACETOPHENONE,
ETOH', AMYL ALC., ACOET, AND ACOBU IS GIVEN. ELEG, COND. OF 1 If4 EOH OR
CONCOo AQ. SOLNS. SHOWS THAT THESE SALTS ARE 3:1 ELECTROLYTES AND THEY
DECOMP* ON DILN. THE ANION HAS NCS rOOROINATED YiA N1. (0ELTA(fiCS,
-1
EQUALS.490, NU(CS) 825, AND NU(CPJJ 2050 00 C:M PRIME NEGATIVEI)o I
DECOMP. GREATER THAI 180DEGREE-S-
N