SCIENTIFIC ABSTRACT DYAKONOV, V.D. - DYAKONOV, YE.G.

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SCIENTIFIC ABSTRACT
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22319 S/133/61/000/004/Oi5/015 Vacuum treatment of open-hearth furnace... A054/A127 inge made from vacuumized ShKh15 steel increases by 70%. Rejects of the steel grade -)80thOA68KhMYuA) due to surface rejects could be reduced from 14.0 to 6.45% by vacuum treatment of the steel in the ladle. No flake formation could be noticed in3AC(37KhS)steel, which also was vacuum-treated. At the Chelyabinskiy metallurgicheskiy zavod (Chelyabinsk Metallurgical Plant), vacuumized siphon pouring was applied in the casting of steel ingots of thelgXHBA 68KhNVA)steel gradeq weighing 1,15 kg. Improved ma-.rostructure and reduced reject rates due to intercrystalline cracks have been achieved. Card 2/2 DENISOV, K.N., kand.tekhn.nauk; DIYAKCNOV, V.D., kand.geogr. nauk Machine algorithms for the calculation of equatorial coordinates of sun and stars on electronic digital computers used in navigation. Trudy TSNIIMF 8 no.47:74-81 163. (MIRA 16:12) DIYAKONOV, V.I., student; TSFAS,B.S., dotsent, natichnyy rukovodi-tell raboty Theory of a rural lever-type well. Sbor.dokl.Stud.nauch.ob-va Fak.mekh.sell.Kuib.sellkhoz.inst.no. 1:42-" 162. (MIRA 17:5) 1. Kuybyshevskiy sellskokhozyaystvennyy institut. Yl-iaf t 1.~ilhaylovich, nauc!~P. sct r. (Va,,-tium, is a mag.-cian] ~nkuum .',~ierd-lcv6kce kniz~moe izd-,,-o, 1"li 3-7 C-ill"I.L. 17:8) :-..e~allov (for Fetrov, DIYAKONOV, V.I.; POPELI, S.I. Nonmetallic Inclusions in vacuum-smelted ball-bearing steel during various methods of introducing chromium. Izv. vys. ucheb. zav.; chern. met. 7 no.10:17-21 164. (MIRA 17:11) 1. Ural'skiy politeklinicheskiy institut I Urallskiy institut chernykh metallov. DIYAKONOV, V., III-MI. Trigger pulve generator. Radio no.10:56-5? 0 165. (MIRA 18:12) ..... 11 . ... ... DiYA,..'ONOV, . V., . I.[at..Gen., TURKIN, P., Eng. Col., NIKIFOROV, ~!., Col, and A STOLBOSHINSKIY~ A. Col. Authors of the book "Kura Artillerii" (Artillery Course) SO: N: Krasna Zvezla, No 0,6(7931) Abstract in USA.F "Treasure Island", on file in Library of 1;ongress, "ir Information livision, Iteport No 91260. 1. Dl"Y;P~01'10V -:1,161 2. USSR (6CC) 4. I-IcLutical Astroi)omy 7. Calculation of local time angles of a hepvenly Lody in deterrnining a location from several near meriJian altitudes., il.or. flot, 12, 1,,o. 12, 9. Monthly List of Russian Accessions, Library of Congress, FeLruary_-1953. Unclassified. D'YAKONOV, V. F - "Influence of Computational Errors of Computed Heights on the L cation of the Ship To Be Determined From the Method of Position Lines' Uch. zap. Vyssh. ankt. mor. uchilishcha, No 4, 1953, 47-67 Analysis of the height value, computed from approximate coordinates of the ship, leads to conclision that the table No 27 of the new edition of Navigational Tables (MT-43) is the Most convenient and accurate. A polemic with P. P. Skorod-Lunov is added, deJing with his work "The Choice of Number of Places of Logarithmic Tables' Used for Computation of Heights of Celestial Bodies," in which he advicies five-place logaritluis for the said computation, while the author considers four-place logarithms sufficifflit. (RZhAstr, No 10, 1955). SO: Sum-110. 787, 12 Jan 56 f. DITAKONOV, V., dotsent. Sextant with optical reading and star finder (from "Ezhamestachnyi zhurnal tochnoi makhaniki i optiki" no.2, 1954) (MIRA 10:11) 1. Kafedra morekhadnoy astronomii Leningrndakogo Vy9shego inzhenernogo morskogo uchiliahchn. (Germany, East--Nautical instruments) DIYAXONOV V.K.- DOROSHMO, NA.; KOKPAIMYRTS. A.I.'; TSARMO, A.P., IIU, G.P., tekhnicheskiy redaktor. [Organizing the work of locomotive crews using Job designation time schedules on the Southwestern Railroad Line] Opyt organi- zataii raboty lokomotiv"kh brigad po imennym raspisaniiam na IUgo-Zapadnoi doroge. Moskva, Goo. transp. shel-dor. izd-vo, 1954. 75 P. (MLRA 7:12) (Railroads--Train dispatching) (Locomotives) D'YAXONOV,,,..V.F.; KULIKOV, D.K.. redakt or; VOLCHOIC, K-M-, takhnichaskir 1* or (Determining ship's position by the sun; with an investigation of accuracy] Opredelenie meste, sudna po solntsu; s issledovaniem tochnosti. Lenlngradj Goo. Isd-vo vodnogo transporta, Leningrad- skoe otd-nie, 1954. 173 P- (MLRA 7:10) (Navigation) DITAKONOV, V., doteent. New dometic instruments for precise time-keoping. Mor.flot 15 noo41 8-10 AP '55. (MLU 8:5 ) (Chronometer) AL BASHTANNIK, Kirill Georgiyovich [deceased) -~ DITAXWOV,~X.X.,. nauchny7 re- daktor; SATCHEEKO. K.H., nauchW redattor; ITAHOV, K.A., redaktor i-datellstva; TIKHOYOVA, Ye.A., takhnichaskiy redBktor [Nautical astronomy) Morekhodnaia astronomits. Moskva, Izd-vo "Horakoi transport," 1956. 318 P. (KLRA 10:4) (Nautical astronomy) T)."Y /~ f ~--C A; C, (~ C " r, RACHKOV, Anatoliy Antonovich; Jk~YAKOXOV,-.V,F.-, otvetstvenW red.; KUZNETSOV, A.D., red.; DROZHZHINA, L.P., tekhn.red. LPrinciples of nautical astronomy] Osnovy morekhodnoi astronomii. Izd.2-oe, perer.i dop. Leningrad, Izd-vo "MorBkoi transport." 1957. 313 p. (MIRA 11;1) (Nautical astronomy) AUTHOR: --*akonovt V*F* 33-3-23/32 TITLEt The eff eat of diurnal aberration on the accuracy of do-i, .1.tezq4n&ng latitude from observations of Polaris (0 vliyanii .sutoolihoy aberratsii na tochnost'opredeleni7a ;hirot-Y mesta po pol7arnoy zvevde) PERIODICAL: "Astronomicheskiv Zhurnal" (Journal of Astronomy), 1W-751-34, No.3, pp. 48 ? (U.S.S.R.) AASTRACT: An analysis is made of the effect of diurnal aberration on the equatorial co-ordinates (a, 0 ) of Polwis and on the accuracy of determinations of latitude of astronomical pobitions of class II from observations of Polaris. This is contrary:to the view of A4'V. Butkevich, who expressed the opinion that this is not necessary. On the basis of the analysis, and numerical tables, the author has shown that the effect of diurnal aberration can eause a total arror of the order of 0-5" in the latitude (with t < 960). It is therefore recommended that the effect of Car&1/1 diurnal aberration should always be taken into account when determinations of the geographic latitude from the observations on Polaris are ca=ied cat. Mere are 4 tables and 4 refeze- hi h re Ma Vic. all of z July 2 1 1'59. LibruT of Congress V J///~ (ilv c 1'~ V, DIYAKONOV, V., dots. Limits for replacing the parallel of an observed latitude and the meridian of an observed longitude by the celestial line of po- eition. Mor. flot 18 no.1:4-5 A 158. (MIRA 11:1) 1. Kafedra morekhodnoy astronomii Leningradukogo Tysehego inzhe- nernogo morskogo uchilishcha. (Nautical astronomy) DIYAKONOIT, Tasiliy Yomich; KUZNICTSOV, A.D., red,; DROZHZHIN&, L.P., tekhn. red, ' ' - - I Determining a ship's positIon by the sun with a check for accuracy] Opredelenie mesta sudna po solntou o*issledovaniem tochnosti. Leningrad, Izd-vo "Morskoi transport,"'1958. 238 p. (MM 11:7) (Navigation) (Nautical astronomy) 20(1,5) PHASE I BOOK EXPLOITATION sov/2o16 D'yakonov, Vasiliy Fomich Morekhodnaya astrono'miya (Nautical Astronomy) Leningrad, Izd-vo "Morskoy transport," 1958, 462 p. 8,000 copies printed. Errata slip inserted. Specialist Ed.: A.F. Matsyuto; Ed. of Publishing House: Z.S. Frishman, Tech. Ed.: 0.1. Kotlyakova. PURPOSE: This textbook on nautical astronomy is intended for students of navi- gation at the intermediate level of naval schools. It is approved as such by the MMF (Ministry of the Navy). It may also serve as a practical manual for navigators of the transport and fishing fleets. CWERACM: This book on general nPtutical. navigation is divided into three sections. Section I contains information from plane trigonometry and spherical trigonometry pertinent to the science of na-vigation6 Section II deals with the fundamentals of spherical astronomy as well as information on the theory of errors. Section III confines itself to -hro problems: determining the position of a ship and compass corrections baL96;d an the observation of celestial boltes. All sections Card l/ 14 Nautical Astronomy S(T;12016 contain teat problem3 to be referenc.,! to the 1957 NwItical. Astronomical Almanac. 111he author thanks navigation-engineers Katin, G.O. Mitsevich, L.S. Golifoov, and A.F. Matsvimo for their help, ~-Iere are 'T2 Soviet referencee. TABLE Or, CONTENTIS: Foreword 3 Introduction 4 SECTI(V I. FUNDMONTAT~j C,? SFIfVP-ft','AL GF,)Nff,;Vlw ANO 111-RICION0~2TR7 Ch 1. Basic Information on Plarie Trigonometry and oi 'lie Theor-y of Logarith a 1. Determination of the trigoaami-tric fti-netions of an acute angle and the basic formulae in plane trigonometry 15 2. The trigonometriz functions of small angles 2k 3. Basic formulae ewpr,~~sstng the relatJorship among the elements of a plane trianglr-. 'It, - 3ol~-.tion of rIWhI.-qnd oblique- angleJ. ffirtngles -- 27 4. Reverse circular Punctton,-~ 29 -5~-- Basic information on the the~)jy of logarit'~Lms 30 Card 2/14 Nautical Astronomy 6. Tables for natural values and the logaritbmic tables for trigonometric functions 7. IDgarithmic tables for sums and differences Ch. II. The Basic Data on Spherical Geometry 8. Basic determinations and principles 9. The spherical angle and its measuremedt 10. The spherical triangle and the corresponding trihedral Basic properties of a trihedral angle lls Polar triangles and their properties 12. Basic properties of the sides and angles of a spherical Ch. III. Spherical Trigonometry 13. Basic formulae of spherical trigonometry 14. Right spherical triangles and their solution 15. Quadrant spherical triangles and their solution 16. Solution of oblique-angle spherical triangles 17. Elementary spherical triangles and their solution SOV12016 34 36 38 40 angle. 41 42 triangle 44 46 51 54 55 59 Card 3/ 14 Nautical Astronomy SOV12016 SECTION II, FMAMENEUS OF SPHERICAL ASTRONOW Ch. IV. Determining the ~position of celestial bodies on the auxiliary celestial sphere 18. The celestial sphere, The basic points, circles, and directions of the celestial sphere 62 19. Basic systems of spherical coordinates of celestial bodies on a celestial sphere; principle of sidereal time 67 20. Construction of a celestial sphere and the graphical solution of problems on a sphere 75 21. The polar or parallactic triangle of a celestial body and its solution by the basic and transformed fonmdis of spherical astronomy 77 Ch. V. The Visible Diurnal Motion of Celestial Bodies 22. The visible diurml motion of celestial bodies and its explanation 85 23. Specific features in the visible diurnal motion of celestial bodies for an observer on the equator and on the pole 89 24. Basic problems related to the diurnal motion of the celestial bodies 92 Card 4/14 Nautical Astronomy SOV/2016 25. The nature of variation in the altitude and azimuth of a celestial body, due to the diurnal revolution of the celestial sphere 96 26. Eypltuiation of the visible diurnal motion of celestial bodies by the Earth's rotation around its axis. Proof of the Earth's rotation 100 Ch. VI. The Annual Motion of Sun 27. Pher-onena confiridug the annual motion of the S~m among fixell stars 105 28. Detcrmin'l~ the path of the Sun in relation to the equator. The eciiptie. "The course of the Sun along the ecliptic 106 29. 'The eally"41c v3tm of coordinates of the celestial bodies 112 30. '"The ni-anue-c of measuring the longitude,, right ascensionand declinatio--, of tfae Sun. The approximate computation of P and OC of the G-= on a glven day 113 ABt7omom~cpl phe--~=ena releted to the visible diurnal and annap'Ll mot-ion the Sun,, for observers located at various latitu(le3 on the Ba-rthls surface 127 Card 5/ 14 Xtmticul Aatron~xW SOV/2016 32. An e--planwi'lon of i3easone.1 changes 124 33. The ra=al Paxvj-Iw% and the aberration of light as proof of the ~,iEvi-Uhls ::wfolvtion arowid the Sun 128 34. 111ne princip-le of! 4eplerfs laws and of Newton's lav of w-li-m::Lial, gra'r-ItFv,..t on 133 35. The principle a-Z praoession anI nutation 135 Ch. VII. The P--r-ye:- Motloz of Moon. and Planets 36. An explans!tion of the proper motion of the Moon 142 37. Pheses o2' the Moon. A&, of the Moon 146 38. Principle o-," aol sx Pn(I luna-- eclipses 149 39. Proper motions of plane-Cs 152 Ch. VIII. The Meaeuxement of Time 40. General considerations on measuring time 157 41. The sidereal day. Sidereal time. Basic formula for sidereal time 159 42. The true solar dV. True actual solar time 162 43. The mean Sun. The mean day. Mean solar time. The time equation 164 Card 6/14 Nautical ABtronoM BOV12016 44, System of ,~ironology. The principle of the Julian (old style) and the Gr!gorian (nev style) calendars 168 45. Time on ditferent meridians. Conversion of time from one meridian tj another. local time. Greenwich Standard Time 171 46. Zonal time, Ship's time and decree time. Switching from local to zonal, jAps, and legal timejand viceverea 175 47. The internitional Date Line - the time demarcation line 179 48. Relation bi!-.veen the sidereal and the mean values of time 180 49. Instrumentii used on ship for measuring time: chronometer, clock -.-;op-watches ', and i 183 50. The correci;:.o.-. of the chronometer and clock. Estimation of Greenwich ~'--;andard Ume 193 51. The rate of chromometer and clock. The diurnal rate and its determination 199 52. The effect of taorperature, atmospheric pressure, hiuaidityjand other factors on the rate of a chronometer 200 53. Time service organization on a ship. Checking the clock by a chronometer. The chronometric journal 205 54. The maritime astronomical almanac, its arrangement and use 210 Card T/14 Nautical Ai3tronamy Ch, IX. Study of the Sky. The Star Globe SOV12016 55. The sky. Brlf.ghtness &nd designation of stars. Constellations 227 56. Description of the sXy and means for finding constellation and stars 229 57. Pu--pose and rxrrsngement of P- stp-- globe 233 58. Basic pr6blems thet can be solved by means of a star globe 236 Ch. X. Se;~tant. 'Meauurement and Correction of the Altitudes of Celestial Bodies 59. The principle snd description of a navigation sextant 240 60. A brief description of the basic pa---ts of a navigation sextant provided wilth the reading barrel "SN-ZShP" 253 61. Analysis of a sextant. General instrumental correction of a sextant 258 62. Checking a sextant on shipboard. Preparing sextant for observations. Handling and care of rL se:ctsLnt 259 63. Sextant with level and centralizer - "IAS-l" 263 6k. Measuring the altitudes of celestial bodies above the visible horizon with the "SN-WhP"sextant 274 65. Specific features in the measurement of meridional altitudes of celestial bodies 278 66. Specific featr-res in the measurement of altitudes of celestial bodies over the zenith 278 Card 8/ 14 Nautical Astronomy sovl2o16 67- The artificial horizon. Measuring the Sun's altitude with an artificial horizon 280 68. Correction of star altitudes measured above the visible sea horizon 283 69. Adjustment of star altitudes by means of general correction tables 299 70. Adjustment of star altitudes measured above the shore line or above the water line of an auxiliary ship 304 71. Correction of star altitudes measured over the zenith 307 72. Correction of star altitudes measured with a navigation sextant Iry an artificial horizon, and with a sextant with an artificial horizon 309 73. Particular features in the correction of low altitudes of celestial bodies 310 Ch. XI. Brief Information on the Theory of Errors 74. Observation errors.' Systematic and incidental errors.' The main features of incidental errors 1 312 75. The evaluation of accuracy in equAlly exact measurements. Mean square error. Limiting error 314 Card 9114 Nautical Astronomy SM/2016 76. Basic formulae for evaluating the accuracy of various functions of measured values 318 77., Accuracy in the measurement of star altitudes over the visible sea horizon 320 78. Test determination of the mean square error in the altitucle determination of a star above the visible sea horizon 322 SEMION JU . DEVEFaMTKNG THE COMPASS CORFOCTION AND THE POSITION OF A SHIP AT SEA Ch. XII. Determining the Compass Correction 79. General considerations regarding the correction of a compass by astronomical observations of celestial bodies. Selection of a method of observation- 327 80. Determination of a compass correction. A.P. Yushchenkols tables 331 81. Determination of a compass correction from k.s. Yurlyev's tables 333 82. Determination of a compass correction by the North Star 337 83. Determination of a compass correction for the moments of the visible rising and setting of the upper edge of the Sun 339 Card 10/ 14 Nautical Astronomy sov/2oA Ch. XI31. General Considerations in Determining the Geographical Coordinhtes of a Ship at Sea 84. Relation between the position of an observer on the earthla.wArface and the position of his zenith on the celestial sphere. The zenith's coordinates 342 85. Principles of the separate determination of the latitude and longi- tude of a ship's position 344 86. A combined method for determining the latitude and longitude of a ship's position. The most favorable-conditions for a combined determination of the latitude and longitude of a point 346 Ch. XIV. Determining the LoQation of a Ship at Sea According to Equal Altitude Lines 87. Graphic solution of the problem by two altitudes on the globe; printiple of aetrographa 348 88. Principle of the method of determing the location of a ship by equal altitude lines. Various methods of plotting the position of an altitudinal line on a Mercator map 352 89. Plotting equal altitude lines on the map from the -point of issue. The elements of the altitude line of position 356 Card 11/ 14 Nautical Astron=y savl2o16 90. Basic means of computing the necessary altitudes and azimuths and their comparative evaluation 357 91. Analysis of the formulas for signs and establishing the identity of the azimuthal quarter 363 92. Procedure for plotting the altitude lines of a position on paper 364 93. A general case of determining a ship's position by observations of two stars, with reduction of altitudes to a single zenith 367 94. Determining a ship's position by observing three stars. The error triangle. Determining the probable position of a ship 371 95. A general case of determining a ship's position by observing the Sun at different times 378 96. An"Ang the nomracy of determining t1ie ship-at-ses, position by the altitude lines 384 Ch. XV. Methods of Separate Latitude and Longitude Determination of the Ship-at-Sea Position 97, Determining the latitude of a position by the meridional altitude of a star 395 98. Determining the latitude of a position by near-meridional altitudes of stars 398 Card 12/14 Nautical Astronomi sov/2o:.6 99. Observation limits for near-meridional altitudes 405 100. Determining the latitude of the ship's position by the altitude of the Worth Star 407 101. Determining the longitude of a position by the altitude of stars 410 Ch. XVI. Particular Cases of Combined Determination of Latitude and Longitude of the Ship-at-Sea Position 102. A particular case for determining the position of a ship by two stars, one of which is the North Star 414 103. A particular case for determining the position of a ship by observing the Sun at different times when one of the Sun's alti- tudes is the meridional altitude: a) morning - noon, b) noon- evening 417 104. Determining the position of a ship by similtaneausly observing Sun and Moon 420 105. Determining the position of a ship observing the Sun, star, or planet at differe4t times 423 106. Determining the position of a ship by the altitude line of a star, and the direction of land object., or by radio direction finding 425 Card 13/14 - Nautical Astronomy sov/2oi6 107. Determining the position of a ship in the tropics with altitudes of the Sun exceeding 88" 426 108. The meaning of a single line of pos:ftion 430 Ch. XVII. Principles of the Structure of the Solar System and of the Universe 109. Basic information on -the, structure of the solar system 432 110. The world as conceivecl by the ancients 442 111. Copernicus I heliocantric system of the Universe 112. The concept of the. structare and evolution of the Universe 445 113. The basic cosmogonic hypotheses on the formation of the solar system 447 Supplement 1 455 Supplement 11 454 Supplement 111 456 AVAILABIE: Library of Congress Card 14/14 144/mas 8-11-59 DIYAKONOV, V.~'dots. Pockot oextant. Pbr,flot 19 no.l'-)~~45 Jit '59. OIRA 12:3) 1. Kafedra morekhodnoy astrononii Leningradskogo vysshego inzhonernogo morskogo uchilishchn im. admirala Makarova. (Sextant) DITAKONOV, V., dotsent Yugoslavs tables of altitude and azimuth of celestial bodies. Mor. 20 no.8:42-43 Ag 160. (MIRA 13:8) 1. Leningv~dskoye vyssheye inzbeziernoye morskoye uchilishche im. admirals. Makarova. "Yoslavia-Hautical astronomy) D'YAHNOV, V.F., dotsent -- Devices for direct deternination of the latitude ;,rd Ion~~itude of the observer. Biul. tekh.-ekon. inform. Tekh. upr.Min.mor. f-lota .'- 79-86 -6-0. OVIIZA -15.1) 1. Leningradskoye vyssheye inzhenernoye morskaye uchilishche irl. admirala Makarova. (Nautical astronoiV) DIYAKONOV, V.F., dotsent, kand.geograf.nauk Direct computation of geographical coordinates of the position of a ship by the observation of two stars. Sudovozhdenie no.2:19-26 162. (MIRA 17:4) 1. Kafedra astronomii Leningradskogo vysshego inzhenernogo morskogo uchilishcha im. admirala Makarova. DIYAKONOV V.F. ~-17 Precomputation of I:ocal.hour angles, and the inclination of the sun and stars for wW moment,of the;day.durliq-the current year. Infomw abor.,TSNIIKF no.741 8udmokh. i sv* o1 n6.191 52-71 '62o (MIRA 1616) (Nautical astrononq) GOLUBKV, Genrikh Aleksandrovich; D'YAKOTIOV, Vasiliy Fomich; KRASAVTSEV, Boris Ivanovich; MURMMISKIY. Felike Hikolayevich; NASfAY, Napoleon Napoleonovich;YM-,AKOV,.i.G., kand. fiz.-mlatem.nauk, retsenzent; ZHEREBTSOV, M.N.,prepodavatell, retsenzent; RYBALTOVSKIY, N.Yu., prof., red.; FRISHMM, Z.S., red.izd-va; STULICHIKOVA, N.P.J. tekhn. red. [Problems in nautical astronowj] Zadachnik po morekhodnoi astronomii. Leningrad, Izd-vo 'Torskoi trnnsport," 1963. 287 p. (MIRA 37-1) I. Arkhangellskaye morekhodnoye uchilishche (for Zl;erqbt8ov). DIYAKONOV, Vasiliy Fomich; jAATSYUTO, A.F., kapitan da-11ne-po pla. vaniya, red. - (Nautical astronorW] Morekhodnaia astronomiia. Izd.2., pe- rer. i dop. Leningrad, Izd-vo I'Morskoi transport," 1963. 587 P. (MIRA 17-4) 'S , -*-~ of Newt-In's q5'r two n i P. 11 f''-' VL -P-!IAKQNQV,s..-Y.j,Y,P dotsent, inzhener-)Fapitan zapasa How to use the M.A.E. (marine astronomical yearbook] interpolation -tables in calculating hour angles and the declination of celestial bodies. Mor.sbor, 46 no.5:58-60 Yq 163. (MM 16:4) (Nautical astronomy) C, tse nt) ka" na, t*i.,.;r:, 0- the !,,,r rer i ho I i nrl I P- 4 Ilay o;, omen t of iF: -t Ka ACC NR AT6029316 SOURCE CODE: UR/0000/66/000/000/0213/0220, -AU-TH011. D'yakonov, V. Go; Usmanov, A. Go ---------- .ORG: none T1 I LE - Boilin[; heat transfer on a surface with direct hi.Gh frequency heating SOU"RCS: Moscow. Energetichaskiy institut, Teploobmon v elemontakh enorgetichaskikh ;ustanovok installation units). Moscow, Izd-vo Naukaj 1966, 1213-220 :TOPIC TAGS: turbulent heat transfer, heat transfer coefficient, alternating ;electromagnetic field I IABST?.kC-L-. With the application of conventional heating methods (direct current, I Alternating 50 cycle current, steam heating) the temperature of the outside surface of ithe tube, which is necessary for calculation of the heat transfer coefficient, is -calculated by the equation3: n- d, 0 = qi- U11 d. jq (2) 4X d :EC Card 1/2 ACC NR; AT6029318 Illere, t. is the tomperature of the inner surface; t is the temperature of the outer, I In 9 0u ;surfaco is the temperature difference between th knno er surfaces; q in i J, 0 or and out Ithe spocific hoat'/flux; Ain the heat conductivity of tho flow; (I , and din are tho joutsid~--and-!~is-ldo diameters of the tube. However, calculation ofoUo value of I",' by ;Equation (2) leads to a large error, in some cases up to 17.5%. This leads to an I ;error in the calculation of the heat transfer coefficient At i1-.1ith the ain of reducing these errors, experiments were carried out using a high ifrequoncy generator, Type GL-15, with a vibrational power of 8*5 kilowatts, and a :-working frequency of 650 kilocycles. Tests were made with a variety of liquids: lbenzeneAq_t nol ~nethanol., carbon tetrachloride acetone, and double-distilled water* ~~~ua-iled results are given in tabular form. The results demonstrate the effect of a irapidly alternating electromagnetic field on the intensity of heat transfer in the boiling of various liquids. It can be assumed that this effect can be explained by I the interaction of the molecules of the boiling liquid with the high frequency !electromagnetic field, leading to an increase in the number of active vapor formation icenterso Origs art, hass 10 formulas, 3 figures and 2 tableso SUB CODE: 20/ SUBM DATE: 05Apr66/ ORIG REFS 004/ OTH REFS 001 Ccird. 2/2 S/137/60/000/012/ooi/04i A006/AOO1 Translation from: Referativnyy zhurnal, Metallurgiya, 1960, No. 12, P. 60, # 28441 AUTHORS: ..D.yakonov, VJ. Petrov, K.M. TITLE: Vacuum Treatment of Structural Steels PERIODICAL: Byul. nauchno tekhn. inform. Ural'skiy n.-i. in-t chern . metallov, 1959, No. 7, pp. 8 - 14 TEXT: The 38MOAOMMA), 12,\2H4A (12Kh2N4A), U\15 (ShKhl5) and band steels were subjected to vacuum treatment. Seven heats were produced in a 250-kg furnace and the same number in a 130-kg induction furnace. Heats of the first group were vacuum treated during syphon-teeming process, heats of the second group were treated in the ladle prior to teeming. The teeming tempera- ture was 1,6oo - i,6io0c, Vacuum treatment In the ladle was performed for 15 N minutes at a residual pressure as high as 15 - 30 mm Hg. The mechanical properties of Cr-Ni steel were not improved. Only a slight increase in ak Of Card 1/2 S/137/60/000/0i2/ow/104i Vacuum Treatment of Structural Steels A006/A001 12Kh2N4A and band steel was observed. The content of non-metallic impurities de- creasea only in band and ball-bearing steel. In all steels [H] decreased by about I - 1.5 cm3/1oO g, and [NJ remained unchanged. The macro and microstruc- ture were satisfactory. Ye.K. Translator's note: This is the full translation of the original Russian- abstract. Card 212 FETROV, K.M.; DYAKONOVP VOIJ FADEYEV, I.G.; SEI.IENENKO, P.P.; KRYUKOV, L.G.; FriniiEa-u-ciha-stiye: FASTUKHOV, A.I.; SHISHKINA, N.I.; FAZDNIKOVA, T.S.; CHIRKOVA,, S.N.; KARELISKAYA, T.A.,; LOPTEV, A.A.; DZFNYAN, S.K.; ISUPOV, V.F.; DELYAKOV, A.I.; OUDOV, V.I.; SUIOIANj L.Ya.; SLESAREV, S.G.; GOLOVANOV, M.M.; GLAGOLENKO, V.V.1 ISUPOVA, T.A.,- ZYABLITSEVA, M.A.; KANENSKAYA, G.A.; POMIJKHIN, M.G.; UTKIJU, V.A.; MATEVICH, L.G. Vacuum treatment of alloyed open hearth atool. Stall 22 no.2:1-13- 117 F 162, (MIRti 15: 2) 1. Urallskiy nauchno-isaledavatellskiy institut chernykh metallov (for Pastukhov, Shishkina, Pazdnikova, Chirkova, Karellskaya, Loptev, Dzemyan). 2. Metallurgicheskiy kombinat im. A.K. Serova (for Isupov, Belyakov, Gudov, Sukhman, Slesarev, Golovanov, Glagolenko) Isupova2 Zyablitseva, Kamenskaya). 3. 6-y Gosudar- stvennyy podshipnikovyy zavod, (for Pomukhin lJtkina, Manevich). (Steel--Metallurgyi (Vacuum metallurgy) Coll 1 t n s Om I ii!~ v ..8 SOURCE: IVUZ. Chernaya metallurgiya, no. 10, 1964, 17- 21 TOPIC TAGS- vacuum treatment, nonmetallic inclusion, carbon ;teel, chromium additive, quartz, tungEt _qLi additive, ball bearing_attel, chromium alloying ABSTRACT: ~Lacuum treatment',of ball-bearing steel greatly improves quality but the problern, of lowering the number of inclusions has been inadequately studied. TherefOre, the authors under-took a study of the effects of vacuum refining cat-bon steel on inclusions and on their composition by using the method of Cr inoculation. The charge was composed of 150 g sponge iron with 0. 0576 C. 0. 0077o Si, 0. 006% Nin, 0. 0055) S and 0. 0081/o P, and 5 g crushed electrode. Metallic chromium (99. 5% C r) was added in batche's of 0. 5, 1 and 1. 516. Specimens were treated in a Card 1/ 2 L 3976h-65 ACCESSION NR: AP4047334 9, high-frequency vacuum furnace at 1585 C, After the completion of boiling Cr was introduced and the specimeris subjected to furnace cooling. The second methed consisting in charging Cr together with the iron into a cold furnace pro- duced 5016 IeS3 inclusions in the degassed Cr specimens. The content of wustite was 6- 7%, quartz 5376 and chromite and chromium oxide 6076 lower. Cr added to degassed metal produced 0. 050 to 0. 0627o (weight of steel) oxides. An increase in tile amount of Cr did not change the number of inclusions. Orig. art. has:'3 tables. ASSOCIATION: Ural'skiy politekhnicheskiy institut (Urals P61ytechnic Institute?; Urallskiy institut chernykh metallov (Urals Institute of Ferrous Metals) SUBMITTED: OlApr63 ENCL: 00 SUB CODE: MM NR REF SOV: 012 OTHER: 001 pure metal (Cr) /9 Card 2/ 2 , ~ Ui I n z h. FREYDIN, L.M.; GRITSE11KO, 14.1.) PETROV, K.M., lnzli.; D'YA,4U New dovolopmont8 In rooearch. Stall 24 no.74596 J1 164. (MIRA 1821) VLASOV, N.;-.; DIYAKONOVj V,I. -1 . Chromium reduction from chromium-containing furnace patching materials. Ogneupory 30-no.M21-21 165. (MIRA l8tlO) 1. Ural'okly nauthno-iseledovatel'okiy institut chernykh metallov, D IYA , polkovnik meditsinskoy sluzhby; ROMASH, V.M., podpolkovnik maditsinskoy sluzhby; BYKIIALOV, L.P., Inayor meditsinfikoy sluzhby Biomycin in treating pustular diseases of the skin; abstract. Voen.-med.zhur. no.3:77-78 Mr '61. (MIRA 14:7) (SKIN-DISEASES) (AUREMYCIT) KRIVONOS. Fetr Yedorovich; DIYAKOHOV, V.K., red.; POLOTAY, A.M., red. [Railroad transportation as an important branch of the national economy of the Soviet Union; on the All-Union Railroad Worker's Day] ZheleznodorozhnyfL transport kak vazhneishaia otrasli narod- nogo khoziaietva Soiuza SSR (ko Vaesoiuznomu dniu zhelezno- dorozhnika). Kiev. CYb-vo po rasprostranoniiu polit. i nauchnykh znanii USSR, 1957. 13 p. (MIRA 11:2) ~Railroads) I-) , ~' // /N CN C ~'J' 1/-, /~ IGNATIDIV, Alakeandr FedorovichLDIYAKOITOY, TO-K-8.1 otvetstyarinyy red.; TSYPIAKOV, II.V., otvetstvennvy red. [Ifew types of cars for Soviet railroads] Novy V . e tit) vagonov na zheleznykh dorogakh SSSR. Kiev, 1957. 38 P. (MIRA 11:4) (R&Uroads--Cars) ywc !21VO V., V~ WGVINENKO, Ivan Petrovich [Lohvynenko. GCRILOVSKjy, Mikhail Ioeifovich [Horilovolk;yi, M.I.]; DIYAKOHOV, V.K.. red.; Lrumo, Y.K. [I~ycenko, F.K.], redo [Electrification of Ukrainian railroads] Blektr7fikatsiia zaliznyts' Ukrair7. Kyiv, 1958. 35 P- (Tovaryatvo dlia poshyrannia politych- r7kh i neukovykh znan' Ukrainslkoi RSR. Ser. 4, no.1) [In Ukrainian] (mrRA u-6) (Ukraine--Ra ilroade-Blectrification) MONMOV, K.K.; DIYA]CONOV, V.L. Blectrodes for multichannel registration of biocurrents of the brain. Zhur.nevr. i psikh. 59 no.8:1010-1014 159. (HIRA 12,12) 1. Laboratori-ya elektroenteefalografii (zav. - prof. M.1% Livanov) Institute, vyoshe3r nervnoy deyatellnosti AN SSSR i kafedra paikhiatrii (zav. - prof. A.7. Sneshnevskiy) TSontrallnogo institute, usoverehanst- vovanlya vrachey, Moskva, (BRAIN phyelol.) T S~ ITR: Ap,:)oo5401 S/0219/65/0-1/002/0278/02C.0 A. M.; T)Iyakonov, V. L. -1a, oa, romanipulator "or inscrt.'rq,; u'oo,,ro4as Int- the ~3 9 y 7, hur n a ISS-SPv I L~ C) r a 1 m, ne rv e I le nerve coil Inz ca C s 2-ic'. a wa7 9 A~- '~'SS T,~) "IR AP5005401 all ole,~trodos must be insortei a-. --ne qa~ne 'no u-.-,.Il a 'e cted. The electrode s ve 7~ e", -10, f, e 70de i er ro 1 a a a 3 pr 0 v a ri o, n v e t A e t a f) s -:7 - Laboratoriya elektrofjziojop~jj -e yaf 'i k14 "'10scow eI I nost i nayrofizioio:~.-, L'aDoratory of the institute of H-1.1-ter Nlervous a:~J, NeuroPh7,siolocy All SS3R) 30SGP63 EN C L 00 SURI CODE: LS OTHER: 006 c.,d 2/2 D'YAKO.wV, V. If. . . ---, i-ribr., 'Ullcj "; Tool '*~ r 51 :A t i ri,- , " O-t, it 1 1 ri.-t r,;n't :t , 16, 1\~cs- 10-11, 1945 iLq-52059019 DIYAKONOV, V. M. Siukeevakie caverns. Prioroda 41, NI 6j 1952. ..LuLl -u- 7_0 s) -1,.~cs a do-c- On o r ca- lco o" c C', ~,..:,:7 of' a of s':ctch of' tli _c for S 0 AUTHOR- D'yakonov, V. Engineer SOV-1-17-58--4-4/21 TITLEi The Manu-facture of L;ut-,',-ing Tools (Izgotovieniye rezhushchego in- strumen',a) PERIODICALt Mashin~ostroita__-, 19:)8. Nr 4, pp 12--17 (USSR) ABSTRACT3 The tool shop ol the Automobile Plant imeni I.A. Likhachev pro- duces 807b of the Plantis requirements for cutti-.ng tools. The art.isle presents the following informat-iou on the work methznds; technology and devices being used at present in this too! shcpt a special cutting stamp (Figure 1) for cutting tool blanks; the new shape of carb-de too! ends (Figure 2) and the technology of attaching the carbidq tiva4 new thin carbide tips (Table etc, Modernization of the -ertical milling machines of the shop is described in general terms. A special high-.efficiency grind.- ing machine for relieving multiple hobs, designed at the xoo-) shop, is described and illustrated by diagram. This grmnder d~_f- fers from the conventional relieving gr~_nders by the absence of the lead screw. The spindle is moved in axial direction by a cam. There is almost no wear in comparison with that of the lead screws. A particular feature of the grinder is that it reduces the accumulated pitch error,, which could not be achieved Card 1/2 in any other known machine design. There are 7 diagrams and S Ov- 117-5 8- 4- 4/12 1 The Manufacture of Cutting Tools and 5 tables. 1. Cutting tools-ProductiOn Card 2/2 - /-,) ' Y PI /V"?, 41 el V V, /Y - TIKHONOV, A.H.; IVANOV, A.G.; TROYTSKAYA, V.A.; DIYAKONOV, T.N. ~-P"-' ~- On the relation of terrestrial currents and earthquakes. Trudy.Geof.inst. no.25:181-191 154. (MIJIA 7:12) (Seismology) (Magnetism, Terrestrial) F) I YVI)I~'N, V. M. , Cand 1'ech Sci '-- (rjiss) 11.,;L riy o~ stn-;ses in I it! ks of link gearp tdtn cle:irances in ball- arid- socket ioInts tf,.e ve of i nc r i L; i j -, t i i e r e 1b i I i ~,y o " i ts o 1, C-., -n9 19 "'ith CAn of* t-,ailwavs IJSI,. ',-os Or~i-~- r,r L~.:,dn and order of Labor Aed i-annet- Inst, oC Engineers of ;,,ailrt~jci tra-1s.port ir. J.V. Stilin) 1~0 conies ('~L, 2'1-~6, lu,"') - 100 - BAULINJ. I.S., inzho,#__Pl -LN.-..--kiLnd,tekhn.nauk.; USKOVA, O.N., kand. tekhn.nauk.; SHUR., Ye.A.,, inkh.;1KOITYMOV, A.D., inzh.; AF,111ikSIM L.U.., inzh.; EVIJKANOV, A.V., inzh. Investigating the mechanism of rail contact-fatigue damages (defects 82 and 64). V9bt*'TSWII-KP5 21 no*4:27-30 162., WIRA 15:6) (Railroads-Raila-Defocts) I P'YAKONOVj V.N. kand.tekhn.naukj RUBIN, G.V., kanditekhn.nauk; I bi " O.V., kand.tekhn.nauk Electric furnace bath for isothermal hardening. Trudy MIT no.160t27-30 162. (KIRA 1632) (Furnaces, Heat treating) KOI-IMEOV, A.D.; DIYAKONOV) V.N., '2esting the bearing strength of a rail stool under repeated impact stress. Zav.lab. 29 no.8:984-986 '63. (MIFIA 16:9) 1. Vsesoyuznyy nauchno-issledovatellskiy institut zholeznodo- rozhnogo transporta. (Steel-Testing) DIYAKONOVJ, V.N., kand. tekhn. nauk; KOLOTUSHKIN, S.A., inzh. ~ Ultrasonic testing of rails removed from the track. Put' i put.. khoz. 8 no.9:32-33 164. (MIRA 17i11) DAULINO I.S.,, insh.) DIYAK YQV . " ~o kandet-ekhnsnauk Tmproving the quality of standard make raile manuractured frcu Martin steel* Trqxdy M.TI MPS no,292tI66-183 165, (MIRA IWO) DYAKONOV, V.P. Evaluating the effects of dissolved gases on the compressibility factor of reservoir waters as exemplified by fields of the Saratov and Volgograd regions. Nauch.-tekh. sbor. po dob. nefti. no.20sl2- 17 163. '(MIRA 17:6) S11 28/61/000/001/004/009 A054/Al 33 AUTHORS: Kletskin, G. I.; Soboll, N. L.; Dt_,Ta K Rabinovich, V. D.,,and Van Zhu-Yao.- TITLEt Study of processes in cupola furnaces in which part of the coke is replaced by natural gas PERIODICAL: Liteynoye proizvodstvo, no. 1, 1961, 19-25 TEXT: Although several Soviet plants use natural gas for firing fur- naces, there is still a number of problems connected with the replacement of coke by gas. In cooperation with the Mosgazoproyekt Institute the Stan- kolit Plant put a.coke-gas fired 10 - 12 t/h capacity cupola furnace into service last year, wh1oh is equipped for tests. As to the design of gas- fired furnacos, the general opinion is that when fired only by natural gas, the cupola design must be changed radically and should be given a shape re- sembling a shaft or air furnace. When both coke and gas are applied, how- ever, its design has to undergo only slight modifications and, if necessary, the furnace can be fired by coke only. Special features of the furnace con- verted for coke and gas firing (Fig. 1) are the two collectors which feed Card 1/12 S11281611000100110041009 Study of processes in cupola furnac,es ... 4054/A133 air to the tuy~res and the burners, respectively. The tuy6res are moreover arranged only in one row in connection with the considerably reduced amounts of coke and air used. In order to establish the optimum height of the bur- ner assembly, twelve burners were mounted in the test-cupola in three rows, the first at a height of 770, the second at 1,070 and the third at 1,370 MM from the axis of tuy6res. At the simultaneous combustion of gas and coke the regulation and distribution of the blast between tuy4res and burners is very important. With the collectors (4, 5 in Fig- 1) which operate in com- bination with independent fans, the required constant gas-coke.ratio in the cupola can be set and maintained. Complete burning of the gas outside the shaft is obtained by a special tunnel-antechamber for the discharge of the gas-air mixture from the burners. The most suitable burner for cupolas fir- ed with mixed fuels is the double-circuit type, in which the gas and the air can be pre-mixed and the outlet cross section is such that -lie speed of the outflowing air-gas mixture is more than 40 - 50 m/sec. During snielting in the cupola furnace the parameters of gas and air consumption for tuy~res and burners change constantly. The control panel Fig. 4) has push buttons con- trolling the slidevalve mechanisms (16, Fig. ~, the push button for stop- ping the cupola operation in case of danger, ~17, Fig. 4), a button for au- Card 2/12 511281611000100-110041009 Study of processes in cupola furnaces... A054/A133 dible and one for light signals (18,'20, Fig-.4), a safety-release button (19, Fig. 4). In order to maintain a constant gas pressure before the bur- .ners and-to ensure the combustion of gas at a given ratio to air, two jet- regulators from the Kharlkovskiy zavod Teploavtomat (Kharlkov Teploavtomat Plant) are mounted, one controlling the,gas pressure (8, Tig- 4), the other the gas-air ratio (9, Fig- 4). The controlling pulse is given to the prea- sure regulator when the gas pressure before the burners attains 0-27 atmo- spheres. The change in pressure before the burners is compensated by a valve (operated by aCK-80-15 = SK-80-15 servo-motor)-, moving before the'burners in the required direction-to equalize the gas pressure. The gas-air ratio .regulator-receives pulses of pressure drops from a diaphragm which controls the gas and air consumption. (differential type A113M(DPIM) pressure gauge). Air consumption of the tuyires--and burners is controlled by an '. -610 (E-610), gas consumption-by an 9-612 (E-612) device.- In order to prevent gas-explo- sions,, a r7K-100 (FK-100) safety valve, designed by the Masgazproyekt,As mount'ed in the gas.conduit; it is equipped with an electromagnet whose head is connected to the air-collector of the burners through a pulse pipe. When the air~pressure drops below a certain value, the gas supply is switched off automatically. When the gas pressure drops below 0.15 atm, theCTIAC-1-5 Oard j/12 S/128/61/000/001/004/009 Study of processes in cupola furnaces ... A050,133 (SPDS-1.5) gas-pressure indicator (12, Fig. 4), starts operating and-the gas-supply is stopped.. The operation b'f all these devices is signaled by a flashlight (20) and a howler (13).. The air-oolleotors are provided with valves to prevent their destruction in-case of explosion. The smelting pidoe'ss, the quality of metal smelted in a mixed-fuel oupola and the compo- sition of the combustion products were stud-ied with various rows of burners (I, II, III) ana also with different combinationalrespectivelys at the.same time I-II,M-III, I-III and all three. The other oonditions of the pro- cess (composition of the charge, for 0 24-44 (SCh 24-44)iron,.. firing. con- ditions and temperature,-etc.) were identioal,,in all-tests. It-was-found that by charging 100 kg coke and 30 m3 gas into the furnace for I ton iron, 875,000 kcal heat was introduced, as against 992,000 kcal of heat used for 'the same amount of iron in furnaces fired by coke only. This can-be ex- plained by the fact that less heat is spent on slag formation due to the de- crease in the amount of flux applied and to the improvement of heat transfer to the charge In the cupola furnaces, partly fired by gas. An analysis of the gas composition in coke-fired and coke-gas fired cupolas showed that the C02/CO ratio is higher-in the latter type of furnaces. It was found that by mounting the-burners higher in the furnace shaft the C02 content of furnace Card 4/12 S/128/61/000/001/004/009 Study of processes in cupola furnaces... A054/AI33 gas.es-incre4ses while ;the CO 'content deciZeases. ,The hydrogen content.also increases in furnaces with mixed fuels (it.is 2 - 2.5 7o, three times more than when firing with coke alone)... Thehigher the bi;rners are placed, the higher the hydrogen.content. Figure.7 presents thq temperature conditions of mixed-fuel cupolasand shows..that they are 150, !, 3000C higher than those in coke fired furnaces. At a level of 3 m from the tuy~'re the temperature of separating gases attains 9,500C it the ooke-gaa furnaoe,.(when row I of burners is operating), while the corresponding temperature for. coke-."ired furnaces is 650 - 7000C... Thus, the smelting of the.rietal charge begins at higher levels in the colce-gas. fired- furnace-,,. As to -.he behavior of carbon, silicum and.. magnesium., no change is. found -in iron.smelted in mixed-fuel ~ou- polas, while the sulphur-coTitent decreases by 0.01 - 0,102 %. Whon the bur- ners of the upper-ro% are used, iron shows an increased tendency to form,ce- mentite and.shrinkage cavities, while i-ts flu 'idity saems to decrease. More- over', iron produced in mixed-fuel furnaces has a higher hardness (by,10 - 15 Brinell grades) while the mechanical properties do not change. The lining of mixed-fuel furnaces requires more frequent repairs since it burns higher up. The coating consists of 35 %6' sand, 25 % refractory clay and 40 Op waste of fireclay bricka. Especially-the coating of gas-burner tunnels has to be Card 5/12 S11 28V6.1;/000/001/,004/009 Study of processes in cupola furnaces... A054/A.133 in perfect cor-dition,. because the regularity of the goemetrical form of the tunnel greatly affects the intensity of gas combustion. Coating with fire- clay blocks was too expensive, a refractory mass is therefore used. The o- pe'ratioa conditions of the mixed-fuel cupola are given irTable 6. The coke bed is 1,.400 mm high.. When the normal operation conditions are attain- ed, 4urther oper'atton is controlled automatically. The.experience of 14 months of operation has shown that the mixed-fuel cupola works satisfactori- ly with 10 ~o coke.for 300 =3/hour. gas, at an air consumption Of 5,000 mm3/ hour.,.producing,10 tona.of-lron.per-hour at a temperature of 1!,4300C in-the chute'.. The output-of the,mixed-guel-cupola is Increased by-20 , 25 % a2 compared.with coke-fired capelaa~ There.are 6 tables and 13 figuresi. Card 6/12 study of processes in cupola furnaces ... Card 7/12 S/1 281611000100110041009 A054/AI33 Study of processes in cupola furnaces... Fit-Ure 1: (gontinued) Idixed-fuel cupola furnace 1 - collector; 2 - stand pipe; 3 - burner; 4, 5 - air collectorsi 6 tuy~~re; 7 tunnel; 0 rectangular-seotion container. Horizontal legendi 1 - Ai:~,fop tuye'rea. 2 - Air for burners Card 8/12 S11281611000100110041009 A054/AI33 S/128/61/000/001/004/009 A054/A133 Figure 4: Control devices and automatic system of the coko-gas fired furnace 1 - millivoltmeter; 2.3 .; diaphroonpuy.. sure gaite; 4--millivoltmeter;5 (not given);- 6, 10 - air conswiiption, gauge; 7 - gasometer; 8,-9 - auto- matic jet regulators; 11 safety valve; 12 - contacts indicating the Jas pressure d;rop; 13 - howler; 14 - operating mechanism; 15 - ser- vomoto;I 16 mechanism of slide valves; 17 push bu-tton for stop- ping furnace operation; 18 - sound signal; 19 safety switch off de- vice; 20 - lamp. Vertical le-end: -to the power line of fan . U Card 9/12 Study of processoo in cupola furnaces ... S/128 61/000/001/004/009 Study of processes in cup6la furnaces ... A054YA133 z4. u F Card 10/12 Figure 7: Temperature of furAace gases Horizontal legend: Conventional cupola, I-II-III row of bur- ners in the coke-gao fired cupola Vertical legendt Temperature of furnace Cases S/12 61/000/001/004/009 Study of processes in cupola furnaces ... A054YA133~ Designation Specification Internal diameter of the furnace shaft . . . . Number of tuye're rows . . ~ . . . . . . . . . . Humber of tuy~res in the row . . . . . . . . . Ratio of tuy~re-section surface to the surface of shaft section . . . . . . . . . . . . . . . Number of burner rows Total number of burners Distance between bottom and tuye-re axis . . . . Distance between the t,,Y~re axis and the lowest row of burners . . . . . . . . . . . Distance between the burner rows . . . Distance between the upper edge of tuy~res and the sill of charging door . . . . . . . . . . . Forehearth-internal diameter . . . . . . . . . 1,300 mm 1 8 10% 3 12 850 mm 770 mm 300 mm 39935 mm 1,100 mm Card 11/12 S/128/61/000/001,/004/Oog Study of processes in cupola furnaces.... A054/A133 Table 61 Operation conditions of cupola fired with coke and gis Time from the begin-' Air in the' t Ydre lAir in the burner Gas Pressure mm ronsump~Preaaure mm onsumP-?res- ning of furnace ope- water oolum ion water colum ion 3ure ion I f ter c-01 "sump ration, min 3/h m3/h nm wa m3/h rR, 0 - 20 250-300 2,500 1 - - - - 20 - 30 500-600 3,500 900-1,000 3,000 2,700 300 30 and more 1700-800 5,000 950-1,050 3,000 2,700 300 The pressure should be raised until the pointer of the gage does not move from 0. Card 12/12 "!;, ~*. I., Parld. Wkhn. n'a'uk; SlYlUiRCHU, teklin. wilik; . .:j :) . , , T Btf;j';'lf!PAV(!V, MI., 1-nzh.; S01101.1, N.L., I 'Y" ' " Yf; ', , , . . ~; -.. j110;.v, fiftmmjvicff~ V.D., lnzj.,, Mlv I t i ng c,- 4.2 , ist Iron In a coke-oven ga-s-fir-ed cupo!a~ Llt.proizv. o. '. L--4. D 165. 19,;12) n L 26089 -66 EWA(1'1/]W'(I)/ETC f) ING(m) ACC NRs . AP6013504 SOURCE COM UR/0120/66/000/002/0090/0092 AUTHOR: Dlyako.novq.vo ORG: none TITLE: A transistorized step-wave volt Me generator SOURCE: Pribory I tekhnika eksperimenta, no. 2, 1966, 90-92 TOPIC TAGS: transistorized oscillator, electronic circuit, transistor ABSTRACT: Circuits are proposed for a step-wave voltage generator based on two tran- sistors working in avalanche breakdown conditions. The basic version of the generator circuit is shown In the figure by the unbroken lines. Capacitor C, is charged through resistor R0until the breakdown voltage for transistor Tj is reached, when a voltage discbarge'takes place through the transistor to capacitor C2 generating a voltage step on the second capacitor. Discharge of capacitor C1 is completed when the voltage across the collector-emitter section of Tj falls below the threshold voltage of this transistor. A series of discharges of this type causes a stepwise Increase in the voltage across 02 which eventually reaches the breakdown voltage of transistor 72- Capacitor C2 then discharges until the threshold voltage for T2 is reached and the process repeats itself. This means that the voltage step-wave begins at tha thres- hold value for T2 instead of at zero, which reduces its amplitude. This may be avoid- Card UDC.0 621.373.5 -'L 26089-66. ACC NRi 'AP6013504 - - 5 T, 0 v 2 . 4 . P422 ~ f F OIA+PU+ T H7 2 2 ~ (or C2 110 2F , . 30 - 0 E s7o-loo OJ- ig;~rjl.. tXro-notstorized g;l-_mp-Tp Sug cor: 091 gengi;#qqTr,. ~001 Card :2/3 L _;kO89-66 FXC-C NRt AP6013504 .2- ed by using the modified circuit shown by the dotted lines In the figure. The diodes isolate the negative pulse formed during discharge of C2, and the transformer then feeds this pulse to the base circuit Of T2 thus triggering this transistor and instan- taneously dischs~rging the capacitor to zero voltage. Formulas are given for calcu- lating the amplitude, duration and number of steps. It is shown that voltages with step durations of 2 usec to 20 msec may be generated.with amplitudes of up to 50 v and any number of steps. The author Is grateful to G. A. Ali-Zade and Yu. S. Ken- gerlinskiy for discussion of this article and for valuable consultation. Orig. art. has; 3 figurest 1 table, 13 formulae* [141 SUB CODE: 09/ SUBM DATE.i 02haj65/ ORIG R'EF: 002/ OTH REP: 001/ ATI) PRESS.- 1 Card 313. aV AUTHOR: TITLE: S/20 62/002/001/004/016 D299 303 Dlyakonovt Ye.G. (Moscow) On difference methods for solving boundary-value problems PERIODICAL: Zhurnal vychislitellnoy matematiki i matematicheskoy fiziki, v. 2, no. 1, 1962, 57 - 79 TEXT: A difference scheme, called the fractional-step method, is considered. This method was developed by N.N. Yanenko (Ref. 5: Ob ekonomichnykh neyavnykh skhemakh (Metod drobnykh shagov). Dokl. ASS SSSR, 1960, 134, no. 5, 1034-1036). The limits of applicability of the method are defined; a modified version of the method is propo- sed whereby its range is extended. The equation au d2u 62U - - + - (1.1)X at 6x2 ay 2 is considered, on the cylinder Q Z, ;, [0 ._~- t ~__ T], _01 ((x, Card *7~ y): O.-x-, 1,0?.y, lilt 6/2' 08/62/002/001/004/016 On difference methods for ... D299/D303 with initial condition u/t=O = (P(X; Y) (1.2) and boundary condition U/S = IP(X, Y, t), (X, Y) C~- S. (1-3) Let h = 1/11 be the s tep with respect to x and Y; T - the time step. Conditioris (1.2) and (1 . 3) are approximated by VIIJI = qhj, C= Uh, (1,21) VIN = *in) Vjn+0 V(n+'), (i, 1) EH Sj,. (1.3') The fractional-step method consists in setting u I~stem of equa- tions involving the intermediate functions v ij (n+pl~2 Uin+'/,) j_ (i _ G)'A2 X_ J _ U(n), (3A2 XX (j 0+11.) (1. .4) (;A2-vjn+I) + (1 A' -Vij Card 2/7 On difference methods.for ... where A2-v(j - Vi+,.J--- 2vj+ Vv- 1.j XX ht I S12081621002100110041016 D299/D303 0 < a < 1. A'-Vij = - Vi'j+1 - 2vjj + Vij-t hi Eq. (1-4) is rewritten in the form .(E - oTA';) vIo-PA) (E + (I - 0) -rA X (1-5) (E - oTA2,,-) VIn+1) (E + (I where E is the identity operator. System (1-5) Ls equivalent to (E - OTA'-~) (E - c;-rA3 X VV ) (1-7) (E + (I - 0) TAI + -rmrl (E + (I - o) TA2- V, where R(11) is given by an expression; Eq. (1 .7) was obtained by eli- i j minating v ij (n+1/2).,If R ij vanishes for all (ij), then (1-5) and Card 3/7 S120 62/002/001/004/016 On difference methods for ... D299%303 (1-7) are equivalent. If however, R ij / 0, it can be shown by an example that (1-7), (and hence (1 .4) too), does not approximate Eq. (1.1). Thus, one arrives at the following Theorem 1.: For Eq. (1.1) with initial condition (1.2) and boundary condition ul, = 0, the fractional-step method is absolutely stable and convergent, with the mean order of convergence O(T + 0(112); in the case of a nonhomoggneous boundary condition (1-3~, the method must not neces- sarily yield an approximation to Eq. (1-1). The modified method is then set forth. The equation au P" L Lsu + f (2.1) s=1 is consideredp with boundary conditions au am-lu (u, FV' ...' a'VM- 1 )S--- (00 09 ... 1 0) (2.2) C-.rd 4/7 332)() S120 62/002/001/004/016 On difference methods for D299%303 and initial condition U I I-0 T (XII X2" ... I XP)' Here (a. (X,) The difference equation corresponding-to this problem, is (Lhv(n+aIP) + 0 P - IN Vln+(s 0, 2 (2.4) (2-4) V(n+l) _ tn+(S-I)/Pl t(L hVjn+j) + LhVjn+(p_j)jpj) + Thl(-), y P P where L. is a sum of series terms, and Thf is a product of series terms Further, the stability of system (2-4) is considered. One arrives at Theorem 2! The fractional-step method for the system (2.1), (2.2)f (2-3) is (under certain conditions) absolutely stable and convergent with mean order of convergence O(T2) + 0(h); if the equation has constant coefficients, the order of converrence is Card 5/7 S/208/62/002/001/004/016 On difference methods for D299/D303 2 2 O(T + 0(h ). The eqvation Ou P OLA T, (a, (X,0OX. (3-1) a. (x,,. t) > 0; b. 0, is then consideredp'with boundary condition U13 = 0 (3.2) and initial condition (2'.3). Tle corresponding difference equations are set up. The conditions are ascertained for the stability of the difference system* Furtherv a modified version of the method is roposed which removes any limitations on the si n of b8 (in E 3.1)). Eq. (2.1) is considered with conditions ~2.2) and (2131: f The function u(x, t), is called the generalized solution of Eq.(2.1) provided it satisfies certain conditions. It is proved that the ge- neralized solution exists and can be obtained as the limit of appro- ximations which were obtained by the fractional-step method. The ba- Card 6/7 33290 S/20 62/002/001/004/016 On difference methods for D299YD303 sic mathematical apparatus used for this purpose invoives differen- ce- Ilener6y inequalities". The proof proceeds by 1%eans of severnl theorems~ There are 17 references: 12 Soviet-bloc and 5 non-Soviet- bloc. The 4 most recent references to the BnClish-lanGuai-e publica- ti-ons read as follows: J. Douglas, 11. Rachford, On the numerical lolution of heat conduction problems in two and three space varia- bles, Trans. Amer. Math. Soc., 1956, 82, no. 2, 421-439; J. Douglas T. Gall,-e. Variable time steps in the solution of the heat flow equation by a difference equation. Proc. Amer. I-lath. Soc., 1955, 6j no. 5, 787-793; M. -bees, Energy inequalities for the solution of differential equations. Trans. Amer. Tath,, Soc,. la.60, 94y 58-73; 1,1. Lees, Approximate solutions of parabolic equations. J. Soc. In- dustr. and Appl. Math-P 1959, 7, 167-183. SUDNITTED: September 27, 1961 Card 7/7 23823 S/020 ,/61/138/002/005/024 0 0 C111/C222 AUTHORg Ye.G. TITLEs The method of variable directions in solving simultaneous equations of finite differences PERIODICALs Akademiya nauk SSSR. Doklady, v.138, no.291961,271-274 TEXTs The author proves the convergence of the method of variable directionB (Ref. 2 1 D.W. Peaceman, H.H. Rachford, J. Soc.Ind.Appl.Math., 3,28 (1955), Ref. 3 1 J. Douglas, H.H. Rachford, Trane.Am.Math.Soc.,82, 421 (1956) ; Ref- 4 1 G. Birkhoff, R. Varga, Trans.Am.Math.Soc.992t13 (1959)) for the first boundary value problem in the rectangle for V< certain selfadjoint elliptic equations of higher than second order. For equations with separable variables the author gives an estimation of the velocity of convergence. In the square D t O!Ex::5~1 , 04!~y!!~l the author considers the problem 2 2u (b(x,y) 2 22u LIU 2 S(x) 92 + 2 22 u ) +j-2 (y) ?2u x DX ?x dy ?x 9y y (c ~Y2 Card 1/1- 23823 3/020/61/138/002/005/024 T~e method of variable ... C1111C222 'u) (e(y) 32 + f(x)u + g(y)u = h(xgy) (1) Y TX TY U) u 0 ')u - 0 (2) T9 2 a>O , c>O b,d,e,f,g,>~O b ac4O 1 (5) a,b,cie-C(3) ; d,e,C=C (2) f,g(:C(T) vij is defined as v(ih, jh) on the net D h 9 x ih , y jh I h ~ IIN 9 0:~:Ji~-:N . It holds uij = 0 on Sh (4) For exterior points of the equare it holds u 0 and for i,J6 D h\Sh for the determination of u ij one obtains the system Card 216 23823 The method of variable ... S/020/61/13a/oO2/005/024 CI1I/C222 L U 16 -T (b u ) +,A (c uij) - x (ai4- h ij xyujj) + 24 w ijl6xy ij w 116 yy Aj (d, 4 xuij) - 4 'Y (e1 4yuij) + fiUij + giuIJ = hIj where u U i-u 1-1 ui+I -ui I h x i h Let L U (a 4 u 'ay (di/Axuij) + t,u,j x Ij xx i 7x- Ij Ly uij yy- (c14 yyU, 1 6'Y (e1 4)yUii) + gjuij 2L xy uij - 24 Ty- (b 'j Axyuij) - (5) (6) (7) (8) Analogous to S.D. Conte (Ref- 5 s Pa8if.J.Math- 7, no- 4, 1535 (1957)) the author defines the iteration process Card 34 23823 S/02 61/138/002/005/024 The method of variable C111YC222 (L + T' E)u(n+1/2 h (L + 2L 1D~E) u(n) (9) x n ij ii Y my ij (L + Ir E)u~'+')- L u (n) + ,(n+1/2) (10) y n ij y n ij where E unit operator, iteration parameter ; u(n), U(n+l) successive iteratione,u (n+1/2jn_ int-ermediate vector. By elimination of (n+1/2) t follows 8 U 1 [V2E + t' (Lx+ L + L L I u(r'+')- h + [T2 2*V L + LXLY] u(n) (11) n n Y x Y j n xy (n) . (n) (n +1) (n) and U U e ke Be (12) where Ae(n+l [-CI-V + v (L + L ) + L LY] e (n+1) Be (n) n n x y x 'U '-E - 2 T' L + L L ] .(n) n n xy x y Card 4/6 The ffiethod of variable ... 23823 S/020/61/138/002/005/024 C1.11/C222 It holds e (n) . 0 on S. Lemma 1 3 The operators A and B are symmetrical, where (B 0 for N N 2 > 0, where ~o L Tij Tij h J=o Theorem 1 x For a fixed V n>/O the iteration process (9), (10) converges lin the metric B - (B P, 11 q, 112 Theorem 2 s If b Z' 0, then for a suitable choice of tIcn In h In E iterations according to the method of variable directions suffice for tUA determination of the solution of (4), (5). The number of arithmetic operation-e- iN '-~ h-2 In h In 6 . There are 2 Soviet-bloc and 5 non-Soviet-bloc references. The four most recent references to English-language publications read as follows s Card 5/6