SCIENTIFIC ABSTRACT KOMIN, A.V. - KOMISSAROVA, L.N.

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SCIENTIFIC ABSTRACT
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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 2/3 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 1/2 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