INVESTICATION OF THE LOWER OXIDE OF SILICON S1O

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CIA-RDP80-00809A000600350460-2
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RIPPUB
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C
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3
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December 22, 2016
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August 22, 2011
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460
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Publication Date: 
October 20, 1950
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REPORT
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Sanitized Copy Approved for Release 2011/09/14 :CIA-RDP80-00809A000600350460-2 1 CLASSIFICATION CONFIDENTIAL CENTRAL INTELLIGENCE AGENCY REPORT INFORMATION FROM FOREIGN DOCUMENTS OR RADIO BROADCASTS CD NO. COUNTRY USSR SUBJECT HOW PUBLISHED WHERE PUBL~iSHED DATE PUBLISHED LANGUAGE Scientific - Chemistry, silicon oxide DATE OF . INFORMATION 1950 DATE DIST. ~ Oct 1950 Thrice-monthly periodical Moscow NO. OF PAGES 3 THIS OOCUYCN7 CONTAINS IN TORY ATION ARF[DTINO iNE NATIONAL OCi[N St V' SiNt., JI AND liT AS AY[NTO [D. TITS TRANSYa3510N ORITN[ RCYLL TION NIB ITL DD CT TLAN~ I R[RRODU CTION Ol i111! TORN OIII RRO NI [IT[D, IS RPO? suNrLtmtNl IV REPORT N0. SOURCE Doklady Akademii Nauk SSSR, Vol LXXII, No 4, pp 699-701, 1950? INVESTIGATION OF THE LOWER OXIDE OF SILICON Si0 M. S. Beletskiy and M. B. Rapoport Presented by Acad D. S. Belyankin, 6 Apr 1950 ~he importance of the lower volatile oxide of silicon, SiO, in electrothermic metallurgical processes is mentioned in the text aP the article. Potential applications of results obtained in the study of this compound are (1) condensation of silicon monoxide and (2) sub- sequent oxidation to silicon dioxideq~rss a method of d~poaiting a re- fractory coating or of hardening and waterproofing a surface under treat- ment. A table is appended_7 ', s Sanitized Copy Approved for Release 2011/09/14 :CIA-RDP80-00809A000600350460-2 Considerable interest has been devoted in recent years to studying the role of Si0 in the reduction of silicon dioxide, Gaseous Si0 is foamed as an inter- ? mediate substance in a number of production processes including: ferroalloys, silicon, steel products (1), and refractories {2) as well as in silicothermic pro- cesses. Moreover, the importance of Si0 is well established in the electrothermic process for producing aluminum-silicon alloys from natural aluminosilicates (3), where, due to its comparatively high volatility, Si0 exerts and appreciable influ- ence on the final composition of the alloy, altering the ratio of the two elements in the alloy in 'favor of aluminum in spite of the letter's relatively higher vapor tension. Industrial exper.. nce shows that in single-;?and'..triple-phase furnaces, 2.5~, and 7?6y6 of aluminum and x.596 and 22.596 of silicon, r~3pectively are lost `.hrough evaporation. The dae^lopm;:nt of electrothermic procedures and other high temperature pro- cesaes in e*hich Si02 is reduced, as well as several physicochemical and physical investigatfo~hs, have dispelled former doubts concerning the formation of Si0 in the gaseous state in tht purse of these processes. Examination of the molecular spectrum of this compound has bean conclusive proof (4) of that:" However, no conclusive answer has been given as yet to the problem of whether Si0 occurs in the solid state or.~~n condensed form prior to decomposing according to the following scheme: 2510 =-~.S102-}- Si, thus Porming an . equimolecular mixture. CQ.YI`IDEI~TIA~ r DISTTRIBU~TION --I I Sanitized Copy Approved for Release 2011/09/14 :CIA-RDP80-00809A000600350460-2 Attempts.to prove the presence of Si0 in the solid state have, in'the majority formed haveeoftensprovenfthemato bevhighlytdispersed mixturessofssiliconadioxide and silicon. A considerable step forward along this line was the Work done by P. V. Geld (5). He produced Si0 by artifical meyns in vscuum, measured its vapor tension by the molecular discharge method, a+.udied several properties of this compound, and determined its thermodynamic characteristics But in spite of this, up to definite proof ofsthe presencetof thisi~ompound inttheisolidnstate),chavennotve been reliably determined. . Two attempts have been previously made st X-ray analysis of SiO. Investigat- ing specimens in which he assumed the presence of 510, Baumann (6) established,on the basis of their interplanar distances, that the specimens consisted of mixtures oP silicon and cristobalite, and in some cases silicon carbide. Inuzuka has re- ported (7) that a Si0 preparation which he investigated had a cubical crystal lat- tice with the constant s equals 6.4 A. The b~sic cell contained 8 Si0 molecules, and the spatial group belonged to the group Th. Beletskiy and Rapoport made X-rsy snalyses of white formations obtained from the condensation zone of "charge vapors" of sn industrial furnace for fusing silicon onewhichythecintensiveainterferenceelinesrwereavisible. hAdcorrection wasbmaderPord X-ray absorption by the specimens. The results of these analyses are give in the appended table. They indicate the presence of a mixture of substances with average values of their a equal to 5.41 A and s2 equal to 4.34 A. Substances having such constants would~e silicon and silicon carbide. Be assuming that the white substance was a single compound, this substance by X-ray study was found to have a cubical crystal lattice constant a equals 6.36 A, this Figure conforming closely to Inuzuka's. By recalculating Baumann's values for the interplanar distances on the bssis of the moat intensive lines, Beletskiy and Rapoport, with the aid of their own indexes Prom the appended table, determined the average value Por the crystal lattice constant ea equal to 6.35 A; this Figure satisfactorily conformed to Inuzuka's data a.a well as to the data cited above. From these Pi ps Beletaki and Rapoport concluded that Inuzuka investigated gur . , Y a compound which was not S10, but rather a mixture of S1 :wd SiC; in other wor.:e, approximately the same mixture which was studied by Baumann. Completely different results were ebtained by the Soviet authors in the+ inves- tigation of preparations obtained as a result of the reduction oP Si02 by ca; bon or silicon at 1,800? or higher in vacuum, or on the reduction of a mixture of Si0? and p1203 under the same conditions. Several of the properties oP the resulting compound were shown to be very similar to those described by Geld. Beletskiy? and Rapoport's preparation was a yellowish-brown condensate, and Isotropic substance with a refrac- tion index, determined by 0. I. Arakelyan, of 1.,92-1.94. Its density, established with a pycnometer, was rho equals 2.13. By X-ray investigation, its cubical crystal lattice constant was Pound to be a equals 5.16 A. No other type oY interference being observed on the X-ray picture, it was assumed that this compound was obtained in a pure state. Haeed on the figure 2.13 Por the density, Beletskiy and Rapoport calculated that with Pour molecules in the basic cell the molecular kei~tvt bf; the. cGmpound,.i9,.,.?- 44.3, which is very close to the +.heoretical value Por. 510+ The crystal lattice constant determined by Beletskiy and Rapoport is a speeiPie ,.~. ~ i ".i.c characteaistic of S10 is the solid state: caHFO~~~T~~~ Sanitized Copy Approved for Release 2011/09/14 :CIA-RDP80-00809A000600350460-2 Sanitized Copy Approved for Release 2011/09/14 :CIA-RDP80-00809A000600350460-2 I CONI:IDE~IT~A~ BIBLIOGRAPHY 1. Geld, A. I. Kholodov, and N. N. Buynov, Doklady Akademii Nauk SSR, LXX, 4, 195'x: ' 2. C. A. Zapffe, journal Am Cersm Soc., XXVII{ 10, 293, 1946? Rapoport, Tsvetnyye metally, 2, 50, 1946. 4. R. Pirs and A. Gayden, Identification oY Molecular Spectra, 1949? 5. Geld and M. N. Kochnev, Zhurnal Prikladnoy Khimii, XXI, 12, 1249, 1948. 6. H. Baumann, Trans. Electrochem. Soc., L}C70C, 95, 1941. H. Inuzuka, Chem Abstr., }IXXVI, 4001, 1942. ~ppended table follows,] No of Sin- S ecp imen Intensit~r 2r delta hKl a2 a2 ~1 a2 1 Average 2 Strong 3 ~~ 4 Weak 5 Strong 6 ~~ 7'' Very weak 8 ~~ ~~ 9 Average 10 " 37.02 0.096 111 29.15 -- 200 40.05 46.21 0.149 200 -- 18.79 211 40.35 61.55 0.256 202 29.16 -- 311 40.10 73.18 0.351 113 29.26 -- -- -~? 78.48 0.395 (110) 2 -- 18.89 410 40.14 95.49 0.544 113 -- 18.86 (211)2 41.20 102.51 0.605 133 29.30 -- -- -- 106.20 0.636 (120) 2 29.30 -- 115 40.76 122.03 0.765 (112) 2 29`.33 -- 522 40.35 135.97 0.858 115 29.34 -- 611 41.28 CONI'IDEN T ~A~ unitized Copy Approved for Release 2011/09/14 :CIA-RDP80-00809A000600350460-2