SCIENTIFIC ABSTRACT SHULTS, M.M. - SHULTS, P.S.

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CIA-RDP86-00513R001550210005-2
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December 31, 1967
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SCIENTIFIC ABSTRACT
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8h626 Some Problems of the Thermodynamics of S/076/60/034/010/003/022 Heterogeneous Multicomponent Systems, III. B015/BO64 The Relation Between the Changes of the Chemical Potentials of the Components and the Isothermal-isobaric Changes of the Phase Composition that in a change of the composition of ternary two-phase systems along the isothermal-isobaric curxre of the phase equilibrium the chemical potential then passes through a maximum when the molar ratio of the two other components in the coexisting phases is equal. A simultaneous application of equations (1) and (3) permits to establish the position and also the kind (maximum or minimum) of the extremum. of the chemical potential. The authors emphasize that only a joint analysis of the equilibrium conditions and the stability conditions of heterogeneous systems permits to determine the character of the changes of the chemical potentials along the total length of the isothermal-isobaric curves of composition. If one of the coexisting phases may be regarded as ideal the following holds: (dx (2)~ > 0 (4) which means that the total molar ratio dx- P,T,x I - k/xl Card 3/7 84626 Some Problems of the Thermodynamics of S/076/60/034/010/003/022 Heterogeneous Multicomponent Systems, III., B015/BO64 The Relation Between the Changes of the Chemical Potentials of the Components and the Isothermal-isobaric Changes of the Phase Composition of the respective component of the heterogeneous system and its molar ratio in the ideal phase change in the same sense, For a system with an arbitrary number of components the following holds: (k) (k)* C111. (dx~":' 0 if X X X k x_ i_1 i+1 n-1 ~d ~x P.T, ~O M P~T X x x x n n n rL i_e, the chemical potential (the partial pressure of the i-th compon'ent of the heterogeneous system) and its molar ratio changes in the studied k-th phase in one and the same (in the opposite' direction if an addition of the corresponding component to the heterogeneous system leads to an inicrease (decrease) of its molar ratio in this phase, By solving the Gibbs-Duhem equation for each of the coexisting phases Card 4/7 Some Problems of the Thermodynamics of Heterogeneous Multicomponent Systems. III. The Relation Between the Changes of the Chemical Potentials of the Componentf and the Isothermal-isobaric Changes of the Phase Composition x 1)... XW n n-i d1i lxn 2 - 1 -2 -n-1 I dPno (8) X(I)X' I" (r T-1 -2 n( 1XI "'Xn(~L2xn X(,)... X(r) X(r) ,,(I) I'dPn n-2 n -i x n('.) Card 5/7 84626 S/07 60/034/010/003/022 Bol5yBo64 is obtained, so that from (8) and the stability conditions one obtains-equation (9) for the conditions of an extremum. of the ohemical otential of the i-th P component on the isothermal- isobaric curves of hetero- geneous systems, consisting of n components and n-1 phases: i - 8h626 Some Problems of the Thermodynamics of S/076/60/034/010/003/022 Heterogeneous Multicomponent Systems. B015/Bo64 III. The Relation Between the Changes of the ChemicalPotentials of the Components and the Isothermal-isobaric Changes of the Phase Composition X1 Xi-IX;i Xi+l--- Xn-1 [disilp.-r 10, conn . . . . . . . . . . . . .0. (9) X X ixn The practical impbrtance of equation (8) consists in the fact that from the data on the composition of the coexisting phases and on the changes of the chemical potential of one component only, it is possible to determine the changes of the chemical potentials partial pressures and activities- of-all other components of a system that is monovariant and heterogeneous unaer isothermal-isobaric conditions. There are 3 figures and 15 referencess 14 Sovieit and 1 USo Card 6/7 84626 Some Problems of the Thermodynamics of S/07 60/034/010/003/022 Heterogeneous Multicomponent Systems, B015YI3064 III. The Relation Between the Changes of the Chemical Potentials of the Components and the Isothermal-isobaric Changes of the Phase Composition ASSOCIATION: Leningradskiy gosudarstvennyy universitet im, A. A. Zhdanova (Leningrad State University imeni A, A., Zhdanov) SUBMITTED~ November 15, 1958 V\// Card 7/7 S tk-) 06 _3 -riole56-Al205 be?ave like Li + electrodes at pH 3 - 12. (4) This effect oL' Al..O decreases with increasing content of Li 0 in the . - 3 2 .-lass; there-fore, higher Al 203 admixtures are necessary to obtain a Li+ function. The measured values were well reproduci'--le both w th rising anr_ failing DH. The behaviur of lithiu,_~ alumino silicate electrodes is explained by the formation of-lattice points with excessive negative char--es during the introduction of trivalent aluminum in the silicate lattice with the coorainat--on number 4; in these lattice points, the hydroEen ions have no lon~-er a covalent but a: weaker bond. The follo--ving 'nolas + O._LIho-"a,+ + Ka,,+) - 0.50'109[1/(a aXa,+)+ +CX ya:4)~ C~ ~ - J1 H+ a- 2 Card 2/3 5/Oj4/62/000/003/007/010 Study 01' Lne electrode... B101/B166 Thert~ are 7 fi~;.~res and 1 table. The most important ~;nAliSh-lanzua-ge reference i.-3: G. i:,. L. 0. Rudin, J. 14. Casby, Science, 126, 331, 191 S -IJ;-Ijv, ITT Eli JulY 7, 19061 Card 3/3 L-1 I Ii 'COI- x /008/01o A Sh"! I t_~ Belyustin, A. T 1, _-'lectrode T)ro:jerties of sodiuzi silicate glasses containing a r._~:. , tr,,-3 um , o_r i nai um oxi a es C Lenin~;raa. Universitet. Vestnik. -Szeriya fiziki i khi.-Ai, no. 5, 1q,_:,2, 116 - 124 S "--'Lr ~~ nt, eff e c Ls of I'm7las s -f or:.,.in-" and ":-.iodify ing" o.~_ides or. mhe : L~ :unction 11. = f(j-.q) have been studied for sodium. 3ilicate glasses with 22 Nal.0 and with difl"erent concentrations bf Al 205, Ga 03, JIn2- , or 2 S, U3 BaO, by :-_3E~rind the e.:.f of the element Ag!AgCl, 0.1 HCIJ-las b"ffer :~oi_tion IacPjKCl solution, saturated, !Hg. The constant 'K -, ! H32C12; C, = 0 . 1 N or sa 0 NaAl V _olf' the equation (g + log(a H +Ka Na) and the value !C = K /K a were _24 -,A! Nz dete~-t;dint_-d, whert A i~- the constant for sodli,-m al_~izinc silicate -lass, an d K '.he constant for sodium silicatQ glass. Admixin.,:T, small. amounts ,of A12C,3 -ave the curve 2 - f(pq) a stepwise course due to different -Card 1, 4 Oj4 162 3/008/C 1 G Electrodc- pro-jertics of ... B101/B186 bl-in-_in-s o--' the hycroren icns to the SiO and A10 tetrahedrors of the C, 4 4 Slase stracturE.. Al 203 acts as a ti-pical glass former. The range of the Na+ function in the Z-vtz:rsus-~jH curve extends with rising A! 0 content. 0 2 3 Ga 0 also acts as glass former, but its modifying capacity beco=es 2 3 01 + evid,~nt in shi.'Tin-- the transition from the H+ function to the Na function towards pH. It is concluded that gallium enters the glass both as Ga!V (glass formcr) and as Ga VI (modifier). In 2 03acts still less as glass former and sho-..%s even more intensive uodifier action by a wide range of the H+ function. kdmixture of BaO (Tilodifier) to Na-Al giaszes rduces the effect of ~.he second -lass for,aer (Al 0 ), making 'he E'-versus-jil 2 3 'lar c-rves s .;. To those for Na-In glasses. The-d4fference between glass -Por-er and aaodifier can be seen from loa ;_4 =B, Al, ~L . ( = f ( _-2 - Ga, ii., 3). A small X is characteristic of modifiers. Vh e r eare 4 fizures and 2 tables. The most -important English-langLage reference is: G. _`:isv::..-.an, D. U. Rudin, J. M. Casby, Science, 120S, 631, 1957. Card 2/4 '/034 /62/000/003/006/010 Zlectrucb-, properties of ... Blol/B186 Z U 3ITT E L November 27, 19061 Fie. 3. Log?( versus .1.11 okla 0 Na 0 - Al 0 SiO 1 2 L 2 r2 - 2 3 2' Na 201 < 2 5 m. u 1 egO' ; ( 2Na 20 A1203 Sio 2' INa201>25 molej(~; (3) -Na 0 - 3 0, - Sio (4) Na 0 - Ga-0 Sio ; (3)-Na 0 - In 0 Sio 2 2 2 2 2 3 2 2 2 3 2' Card 3/4 W. i,j I S/020/62/142/000'/017/019 3101/B144 An'11GRS Nikol'skiy, B. Corresponding Member AS USSR, isakova, IT. F. , and qnul ts , m. I,,-_ TITLE: Composition of boron alumosilicate --lasses and its effect upon their electrodic and acid properties PERIODICAL: ~Ikaademiya nauk SSSIR. Doklady, v. 142, no. 6, 19062, 1331-1334 TEXT; The present paper vas read at the session of the OS Otdeleniya khimicheski'~-h nauk AN SSSR (OS of the Department of Chemical Sciences of t'e A.S USS-R) oil Miay 30, 1957. It concerns a new method of solving -lass i1 I C, 1~ electrode problems and such related to hyalurgy in general. The electrode Potential as a function of the PH o"' the electrolytic solution was mea3ured or, silicate glasses with a content (riole0,0') of 0-16.3 of B 2 05) 0-2 of A120 3? 0 10-22.7 Of I~a20, and 0-6 .4 of CaO: i~' = L? +--blog(a.. + Ka~ ',a.), where 2 .3RTIF; K - aH' NNa ' /a, is the exchange coefficient between Na+ a and HT+ With increasin- PH, each -lass passed from the hydrogen function Card 1 S/020 to-2/142/006)/Cl 7/019 Composition of boron alumosJlicaze ... -:"J-VI73I,44 0 (,o +,'J~lo- az,.) -Uo the sodium function: + ~jllogKa INa* T 'N' a This results in the relation: -logK log(a,./a A Na' de~o`endence of K on the ratio bet-vieen the strong acids and the sum of stronC and weak acids in the glass was found. -logY is a unique function of the molar part, a, of the stronug acids in the glass: a = I 'I I B 0 + Al 0 /FlIa O(ca) + CaO(~'O)] . The transition from the L 2 3 2 5 j ~ 2 hydroL_-en to the sodium function occupies a wide zone of the diaGram in glasses with a comparable content of strong and weak acids, and a narrow one in Elasses -.-iith a prevailing content of either strong or weak acids (Fi---. 3). There are 3 fi.a-ures, 1 table, and 8 references: 7 Soviet and I non-Soviet. The reference to the English-lanjuaCe publication reads as follows; B. Len6yel, E. Blum, Trans. Farad. Soc., 30, 461 (1934). k'"SOCII31ON khimicheski.v institut Lenin-rads- kojo gosudarstvenno-c-o universiteta im. A. A. Zhdw~nova (Scientific Research Chemical Institute of the Lenin,~;rad State University imeni A. A. Zhdanov) SUBIMITTED: March 11, 1961 Card 2/3 NIKOLISKIY, B.P.; SHULITS, M.M.; BELYUSTIN, A.A. Influence of the nature of the second glass-forming oxide on the sodium and potassium electrode functions of silicate glase-es. Dokl.AN SSSR 144 no.428"-848 Je '62. (MIRA 15:5) 1. Leningradskiy gosudarstvennyy universitat im. A.A.Zhdanova. 2. Chlen-korrespondent AN SSSR (for Nikollskiy). (Electrodes, Glaae) (CIxides) SHITLITS. M.M.; PESIEKHONOVA, N.V.; ROMANOVA, L.M.; ANDRIANOV, A.A. Study of the electrode properties of lithium alun,:inosilicate glasses. Vest. LGU 17 no.16:108--U5 162. (MIRA 15:9) (Electrodes, Glass) NITKOLISKITY, B.P.; SIJLvL?T~, M.N. Some aspects of glass eiectroaq thaor7. 7.1hur. fiz. khir.. 30' no.6t1327-113310 Je'62 (KIRP, 1740) 1. Leningradsk-iy g~-,sud,-Ir5rv,:~nnvy wn-*~Xersltlet. card )/.? --.. -- --- --- M~~ I ---- -- ---- --- - TITLE: PERIODICAL: TEXT Glasses containing 24, 27, pr:,30-'_mole% Li- 0 and an addition of T- 2 . I Ca -0 ud curves tting the plo MgO, or ~ BeO . were :at ied by .20 mole% of BaO, a P11. Results: BaO shifts the upp e H+ function E versu er.limit of th 0-3 pH units into the,alkaline region. In some casest range by 0.1 + ion, also the lower, limit of the B_ -function.~is shifted in positive direct The exchange constant of Li _.'.Ba-glasres::Ls s6mekhzit lower than that of-.!.--.. 0 f e binary glass. CaO addition narr ws i.~e unction rang in-the reasesJ alkaline region, extends the transiti.on~.range by ,A pH unit, and inc Card 113 S/054/63/004/001/012/022 Study of how alkaline earth oxides~ B101/B215 the exchange constant. MgO has the.same effect but much more intensivelyl:-.-%,:~~':_. the shift in the upper limit of the e function caused by 15 mole% MgO*,,.,_t_,_, at 27 mole-/.' Li 0 is 3.3 pH units, but that due to 15 mole% CaO ijr~_Mv 2 3 pH units at no more than 2,.5 unit. The shift caused by BeOis 2 mole%; at'15 - 20 mole/. BeO,"this shift in.d6id direction is 3-4 PH- units. The-effect on the exchange constants increases-as follows: BaO