SCIENTIFIC ABSTRACT CSERNAY, LASZLO - CSERNYANSZKY, H.

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CIA-RDP86-00513R000509410011-0
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S
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100
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July 28, 2000
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December 31, 1967
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SCIENTIFIC ABSTRACT
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VARRO, Vincell dr.; SERNAY, Laszlo, dr. Obaervations on the differential diagnosis of disorders of gastro-- intestinal resorption. Orv. hetil. 102 no,28:3.302-1305 9 JI 16l. 1. Szegedi Orvostudomanyi Egyetem, I oz. Beivogyaszati Minika. (GASTROENTEROLOGY diag) Vol*- 8,-- no. 4t- Apr. -1955 - -j~arnrar -EaarCjjr-azdasa Measuring waste power in the textile Industry and possiblUties of its UtUlzation. P. 152. SO: Monthly list of East European Accessions, (EEAL), LC, Vol. 4, No, 9, Sept. 1955 Uncl. L 37929-66 ACC NIPL. AP6028499 SOURCE CODE: HU/0018/65/017/006/0662/0665' C, -Istvan AUTHOR: Rak, .~lman.e Vargai Laszlo: Krigga, Ferenc--Krizha, F.;_Ss atiZ- ,ah Cherkhati ORG: I. and II. Medical Cliniess kdiqaLUniversity of ~Kje ed ged! Orvostudomanyi Egyetem, 1. es II. sz. Bel~i~k-a) g,_ _.~Sze TITJZ: Effect of human serum protein fractions, separated with Rivanol, on the circulating thrombocyte count of mice SOURCE: Kiserletes orvostudomany, v- 17, no. 6, 1965, 662-665 TOPIC TAGS: mouset protein, blood circulation erythropoiesis, hematology, circulatory system disease, blood serum ABSTRACT: Obtained by agar gel diffusion and separation with Rivanol., thefractions of three patient sera with thrombopoietic activity and two normal sera have been, studied with regard to their effect on the circulating thrombocyte count in mice.. According to the literature and our own exploratory data, the supernatant liquid obtained by Rivanol separation contained only one immune electrophoretically homogeneous A globulint transferrin, in addition to gamma globulin. The whole serum of the patients, the A globulins as well as the Rivanol-supernatant liquids and the majority of-the 13 globulins weremoderately or pronouncedly positive in the mouse test, -that is, they enhanced thrombocytosis. This can be considered a renewed indication of a relationship between the humoral regulation of erythropoicsis and thrombocytopoiesis. Orig. art. has: 1 table. IJFRS: 34tl6l] SUB CODE: 06, 07 / SUBM DATE: 17Feb65 / ORIG REF: oo3 / oTH REF: 008 -FFF -:i oz by M isss B. T. R. Demomwallon of Co- and Andrits A7760 Dec. Vol- 3 EkktMeohnika. V- Apr. 1954 -M.M. Ellootrima Enorhoring p, 5043M. d ennin n1l ten Discuss, Use Of Oficillogal rge begins. esmts results Of SiOn at which COM" it Ov h,ad lisle fittings anti t-n,- ineasurcments carried ins, ph, tables. foraw". Diagrams- -1. lid 1 01 11- 111 v awn ~Itm I h.-vat, 1 1/' CSERNATOMY-IiOFFER, A. (Budapest, XI, Muegyetem rakpart 3, Ungern.) The problem of impact strength of circuit breaker of medium potential inside installation. Periodica polytechn electr 4 no.2:79-95 160. (EM 10;4) 1. Lehrstuhl fur Elektroenergie der Technischen Universitat, Budapest) (Electric circuit breakers) 2:~104 H~007/61/000/005/001/001 DO18/D105 9ql AUTHOR: Cserna'tony-Hoffer, Andrfis, Associate TITLE: The mechanism of corona discharge PERIODICAL: Elektrotechnika, no- 5, 1961, 212 - 222 TEXT: The author presents briefly the available information on the mechanism of corona discharge, deals with the physical characteristics of the partial breakdown developed in the high field surrounding the anode and cathode and explains the criteria for the field-sustained discharge. Literature des- cribes corona discharge as a high-frequency generator in radio and TV inter- ferences and explains its destructive effect on insulators of high-tension cables, machines and apparatuses, but provides no answer to the question why corona discharge can be regarded as a high-frequency generatore On the basis of publications by L.B. Loeb (Ref, 3: "Basic Processes of Gaseous Electronics"s University of California Press Los Angeles 1960), the author investigates the particular characteristics of the corona discharge in air and other.gases. In examining the corona discharge in air starting in the high field surrounding Card 1A 0 21104 H/007/61/000/005/001/001 D018/D105 The mechanism of corona discharge the anode, the author refers to the formula by Loeb -.A 1.66X Inf e e (6) expressing the number of photoelectron avalanches starting beyond the active zone. The process is considered self-sustained when the first avalanche is followed by another complete avalanche, i.e when n f=1. The practical appli- cation of this formula is, however, extremeiy limited, since the knowledge of the f11 f2 andA coefficients is incomplete. The pulsating corona caused by the Trichel impulses at the caPode turns into a continuous corona by in- creasing the potential to ov'er 10 cycles, whereby the amplitude of the im- pulses rapidly decreases. Referring to experiments by Jones F. Llewellyn and G.C. Williams (Ref. 41: Proc. Phys Soc. 66/A (1953) 346) and G.L. Weissler (Ref- 38: Phys. Rev. 63 (1943~ 96), the author states that the initial potential of a continuous corona is not constant. Cathode spots pro- Card 2/'10 21104 H/007/61/000/005/001/001 D018/Dl05 duced by maintaining a discharge for several hours explains the presence of the time lag prior to the development of the corona discharge and the presence of phenomena similar to hysteresis, i.e. that the initial potential of the corona is higher than the potential when the corona ceases. Alost of the ionization occurs as a result of secondary electrons released at the ca- thode by positive ion bombardment. These electrons produce ionization by moving from the strong field to the weak field, leaving a positive ion space charge which slows down the incoming ions. According to Loeb this criterion is valid only for a short transition period of the corona development. With the high field at the anode in experiments on corona in gases the photo- ionization tendency of the gas is determined by the difference between the ionizing energy of the gas molecule and the atom, by the possible. number of the produced metastable states and by the extent of the absorption factor. Weissler, Loeb, Miller and Mohr describe the discharge in clear N29 H29 02qAt and CC12F2 gases. Weissler's investigations proved that in H2 and N2 only Card 3/10 H)too"776h/000/005/001/001 D018 D105 The mechanism of corona discharge continuous corona discharges can occur. The characteristic curves of the initial discharge at the internal anode in concentric cylindrical electrode arrangement in air and.in N2 are shown in Fig. 13 and 14. The increase of ~t he current in N2proves that the avalanche photons which do not reach the cathode in the air, bring about a considerable photo-emission in N In 2- considering the suitability of 02 for photo-ionization, it was proved that the mechanism of photo-emission in 02 is similar to.that in N21- The high absorption of the high-intensity radiation suitable for photo-ionization causes the start of the pulsating corona in 02 directly with "pre-onset streamers" instead of "burst pulses". Pig. 15 shows the characteristic curves of the initial discharge between concentric cylindrical electrodes with in- ternal anode in pure 02 according to Miller and Loeb. Argon is especially suitable for photo-ionizationo while the CCl 2F2gas is characterized by a Card 4/10 I - 21104 U/007/61/000/005/001/001 D018/D105 The mechanism of corona discharge strong electron affinity. In the development of initial negative discharges in the high field surrounding the cathode the electron affinity of the gas is the decisive factor. Due to the low electron affinity of the hydrogen and the negative electron affinity of nitrogen and argonv Trichel impulses Can$ not develop in these gases. Experiments revealed that mixing one of these gases with an extremely small amount~of a gas having a high electron affinity causes the immediate appearance of Trichel impulses, thus confirming the pre- vailing theory on the mechanism of the corona discharge. In gases which cannot produce a negative field charge, i,e. those without Trichel impul5es, the initial voltage is as high as the breakdown voltage, as is the case with argon. Whether H 2 and N2 also have this property has not yet been estab- lished. From the above experiments it became evident that in case of de the corona appears as a source of.high-frequency interference only on small band- width. Since in case of industrial frequency, the potential crosses the bandwidth of the pulsating oorona 100-200 times per second, the partial break- Card 5/1o 2UO4 V/ H/007/61/000/00:;/001/001 D018/Dl05 The mechanism of corona discharge down of industrial voltage.is to be considered as a permanent high-frequency interference. The widespread aosumption that corona discharge can develop only on high-tension overhead lines when the voltage exceeds the critical voltage is rejected by the author on the grounds that the critical voltage of high-tension lines is the-voltage at which the conductor field intensity, as determined by the size and arrangement of the line, reaches the dielectric strength of the air. Breakdowns, causing interference can, however, develop already at sub-critical voltage. There are 15 figures and 41 references: 37 non-Soviet-bloc and 4 Soviet-bloc. The four most recent references to English-language publications read as follows: Loeb, L.B.: "Basic Processes of Gaseous Electronics". University of California Press Los Angeles 1960; Amin, M.R.: J. Appl. Phys. 25 (1954) 210; Amin, M.R.i J. App'~ Phys. 25 (1954) 358; Amin, M.R.: J. Appl. Phys. 25 (1954) 627. Card 6/ 10 21104 H/007/61/000/005/001/001 D010105, The mechanism.of corona discharge ASSOCIATION: Budapesti Muszaki Egyetem NagyfdszU"1ts69u0 Technika bs K6szUl6kek Tansz6k (High-voltage Engineering and Devices Deparl't-Iment of the Budapest Technical University) SUKUTTED: January 1961 Card 7/10 p, 2W4 H/007/61/000/005/001/001 DO18/DlO5 Tho mechanism of corona discharge Fie-"13- I (U) characteristics of the initial discharge between concentric cylindrical electrodes with internal anode *according to C.G. Miller and L.B. Loeb (Ref. 20: J. Appl. Phys.' 22 (1051) 494). Fig. 13. Card.8/1.0 OWNER*= Q m _ gsg .- SIN 01-1- U,~ 211o4 H/007/61/000/005/001/001 D018/D105 The mechanism of corona discharge PiC6 14- I(U) characteristics ofthe initial discharge in pure H2 between concentric cylindrical electrodes with internal anode, according to Miller and Loeb (Ref. 28). Fig. 14- Card 91110 21104 H/00 61/000/005/001/001 D018YI)105 The mechanism of corona discharge Jig, 15. I(U) characteristics of the initial discharge in pure 02 between concentric cylindrical electrodes with internal anode according to Miller and Loeb (Ref. 28). Lxj Pig. 150 Card 10/10 ~g RE H/007/61/000/012/002/002 D286/D303 AUTHORS; Gsernatony-H offer, AndrAs, Associate, Oandidate Horv&th, Tibor, Doctor, Associate, Oandidate of Technical Sciences TITLE: Formation of the initial leader in the lightning stroke and in the laboratory flash-over. Flash- over in air, lightningg lightning protection IV PERIODIOAL; Elektrotechnika, no. 12, 1961, 555-572 TEXT; The article is the fourth in a series and the authors assume that the previous articles are known to the reader. The work done on the subject during the last two decades is re- viewed and imperfections in the theories are jointed out. The theories of Szpor (1942)f Bruce (1944), Loeb (1954), Schonland "Pilot Stzamer'l- theory C1953), Honda modified "-pilot streamer" theory (1957) and Griscom (1958) are described. The authors Oard 1A H/007/61/000/012/002/002 Formation of the initial D286,/D303 state that although the theories agree fairly well with experi- mental results, this is in some instances due to contradictions and wrong assumptions. In SzDar's theory the Use of average. speed is not justified* The assumption that the current in the standing phase is half of the advancing phase value is not jus- tified. Bruce uses a constant which has several different values in the literature. Bruce uses a formula which assumes that a constant corona current leaves the leader which can only flow until equilibrium. is reached due to the radial expansion of the leader. When calculating the radius of the leader$ Schonland takes into account only the charge of the head of the leader and declares the rest negligible. It is also surprising that instead of using Hagenguth's results, Schonland uses values ob- tained from 60 cls experiments. Griscom. calculates that the current reaches 50 KA when the head of the leader expands. He ignores-the fact that a current of this magnitude would result in a substantial light effect. In practice there is no light Card 2/4 'o, 11/007/61/000/012/002/002 Formation of the initial D286/D303 effect-in this phase. According to Bruce's and Schonland's theo- ries the 11 preparing discharge" and the leader progress in turn; also according to Bruce both have the same diameter. Nei- ther of these assumptions is correct. The intermittent progress calculated by Honda does not agree with observations. The dia- cussion of the theories indicates that'they are not applicable to laboratory flash-overs. There are 20 figures and 17 referen- cess 7 Soviet-bloc and 10 non-Soviet-bloc. The 4 most recent references to the English-language publications read as follows: i ii. Hagenguth, A.F. Rohlf, W.J.Degnan, Trans. AIEE 71 111 6952) 455; B.F.J. Schonlandt Proo. Roy.Soc. 220A (1953) 25. Loeb L B hys..Rev. 94 (1954) 227; S.C. Griscom: Trans.AIEE 77 111 919 ASSOCIATION: BudapestimilEizaki egyetem nagyfeezUe.tsegil tech- nika &a kesztila'b&k tansz&ke (Technical Card 3/4 Y