SCIENTIFIC ABSTRACT PIKELNER, S. B. - PIKELNER, S. B.

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SCIENTIFIC ABSTRACT
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PIKLI'f'~~h ;! k =-=0- -.. flial Inveoti,at:cT: (~ ;-LuArescence c,,' Lx I "Cl, 1~"G!-.Cow '--dr-r r,. ' - ', Ir.enl ' . 1. Lo-,rx~rror,-1, ',. "'. . CM, 14 Dec 54) Survey of cienti ,'ic ia.d Tlect.t.~ct-.Il :ds:,ertatl~-r... i~ofonded I* i .,:- i if-I er iAuccticnal ;LnE (I. ,I SC : Six- . 1% c . 5 '3 t- , 2-4 J u1, ~ 5 PinLIMM, S.B. --ft - 00a the distribution of Interstellax matter" (in Xngliobj. G.Alter. Abstract by B.B.Pikellser. Topkosm* 2:325 154. (MBA 8:5) (Interstellar matter) PIKILIMM, B.B. -... "Sow structural characteristics of gas nel"tlas and tbair relation to the stars.0 V.G.Nsemkov. Abstract by SJL?ikellser. Vop.kosM6 2:325-326 954, (MM 8:5) (fthase) (stars) I ~-/ w - /~ ii~5 - Plf,-~~ C FIKILIMR, S.B. wmwimoo~ Kagnetic fields in interstellar space. Vop-kosm- 3:85-93 154. (Magnetism) WaL 80) t i ~~ L- L-, N 1~ NI-,~) ATUR, ~L.H.; - PIXEM Q lm 'Turbulence in the interstellar madlunm[in Zngllshj. Abstract b7 S.B.Pikellner. VOP.kosm. 3:317-318 154. O"A 8:3) (Gases, Interstellar) "I v\ f I -L- !m [ r) , - ~) BLTRS. D.1 SPIT=, L.; PIKELIMM, S.B. OThe density of molecules in interstellar spaceOCin Xnglishl. Abstract bv S.B.Fikellner. VOP,koon. 3:318-319 '54. (Gases, Interstellar) (MIRA 8:3) ~ I )~ i: - t v U t~ . -, "-~ SPITZER. L.; SAVIDDY7. M.; PIE131CLO S B OThe texperature of interstellar matter*[in English]. Abstract by S.B.Pikellner. Vop.kosm. 3:319-320 154. OaaA 8:3) (Gases, Interstellar) (Temperature) V I F, L L'JV LK) - -L . HILTM, W.A.; PIEELIMM, S.B. won polarization of radiation b7 interstellar medium*[in English]. Abstract by B.B.Pikellner. VoP.kosm. 3:320 154. (MLRA 8:3) (Stare-Radiation) (Polarization (Light)) RMOCK, H.W.; PIKB Sa.- -WA 08tol1w -ago tic fieldow[in Xnglishi. AbBtract by S.B.Pikellner. Vop.kosmo 3:321-322 154. Oaft 8: 3) (stars) (magnetism) IlCon'erencp !,evoted tr ~-ysics r Nehi.t v, ind rr IrterF-I't ir -itter" Vor. osmor-ni I Ic,r4p c-161 Yhe crn'erenc- vis --r,r-ein st.rr o f t,'- e 1 1 .':S~. I r s! - rs r i~ ve r,ul7,.;ec* -.-rr, ~rrlar+sur-an, 117e , I I', IrasewslAy, Yi. ~,T-per, V... r-71 r-w-l i v '.e~e ~ ins]- !y r, V., 1 1 - vsl~ i-.,a nd Vn r r, t s -7 1- (R:7fAstr, Ur 1 1 ,ur . Nc If U-) PIM169 MKR, S. B. AltetrouWmtic phenowas in astrooWeles. Usp. "trea.mook 6:281- 322 154. (KERA 7: 8) (magnstism) PIMMITFIRP S. R. "Spectrophotometric StudY of Dif fuse Nebula NMC 7000" Tzv. Krymsk. Astrofi7. Observ., 11, 195", :1p 8-17 The study was carried oiit by means of the nehn-lar spectrof-r-aph of Maksutov- loannisiani design. Relative intensities of 11 and N lines were corr,cted for interstella absorption accordinr to the redenninr of the star HD 19Q579 of class 07 which, as it was pointed out by (,. A. Shayn arid V. F. (,a.-.e id. ,,, of the nebula. Author cor- F to 3, (1951)), excites the lurrLinosit, same conculsion. He also finds dusty a~jsoftinF matter between the Pelican ne~)ula and the star IUM 199OV.1 of class P3. (RZhAstr, No.11, 1951j) SO: 17-31167, 8 Mar PIKELNER, S. B. "Method for Studying 7kirbulence frDm Fluctuations of brightnesc in Neljuiae' , (Theoretical Astrophysics, Diffuse Nabulae), Izv. Krymbk,Astrofiz, CIL,--erv. N4- 11, 1954, PP 311-38 Abs W-31146, 1 Feb 5", PRELINER, S. B. and CHUVAYEV, K. K. "The Probable Mechanism Governing the Luminescence of the Night Sky in the Continuous Spectrum". Izvesti-ya Krymsk. Astrofiz. Observ., U, pp 178-184, 1954. The nature of the radiation of the night sky in the continuous spectrum is considered on the basis of measurements of its intensity, in various regions of the spectrum, which were carried out by K. K. Churayev by means of a photometer with secondary-electron multiplier. It is shown that recombination of electrons in neutral atoms of oxygen leading to the formation of negative ions 0- can give radiation close in intensity to the observed radiation. Such a process can be effective in the F layer of the ionosphere, whiq at night is about 250 km high add which has and elecl6on creentration of nj 2 lo-, cm-3, concentration of neutral atoms of oxygen no 5.10 am- . and electron temperature of T = 1500 . In the expression for the energy radiated per unit volume containing n, electrons and no atoms is the quantity k , which is the coefficient of absorrtion computed for one negative ion. The effectiv thickness of the radiating layer is taken to be equal to 50 km. The computed inten- sity of radiation is close to the observed intensity. Given the quantity T, one can compute the behavior of k as a function of wavelength on the basis of the observed energy distuibution. As it turned out, kv increases from the limiting series toward the side of short wave lengths. The authors evaluate how esgential the other mechanisms of radiation in the continuous spectrum can be. They conclude that the choice of 1/2 Continued: possible mechanisms is extremely limited. Formation of negative ions must lead to strong decrease of ne- Inasmuch as the concentration of electrons and the intensity of luminescence do not decrease significantly in the course of the night, it is necessary to assume that there exists a process that disrupts the negative oxygen ions and restores the number of electrons. It is shown that in this connection electrom collisions cannot be effective. The same holds for heavy particles. The most probable mechanism of disruption of megative oxygen ions is consid1red by the authors to be their collisions with ejdcited oxygen atoms in the state D 2' This conclusion, however, is based on the as5umption that the energy of dissociation of a negative ion is equal to the energy of a ouantum of the red line ,,f night-sky luminescence. Therefore the presented evaluation only indicate6 that in principle mechanism can exist which involve disruption of negative ions. (RZhGeol, No 1.1, 1955) SO: Sum No 884, 9 Apr 1956 2/2 PIKELINER, S. B. "Electron Collision As One of the Possible Hechanisms Governing the Excitation of Night-Sky Radiation of the Red Linen. Izvesti-ya Krymsk. Astrofiz. Observ., 1-1, pp 185-188, 1954. The possibility of the excitation, by electron collision, of the red triplet of oxygen 6300, 6364, 6392 Angstroms which is observed in the spectrum of night-sky radiation is considered. It is noted that form the viewpoint of "selective refraction" one cannot completely explain the very co-iplex character of the behavior of the red line. The rossibility of excitation of oxygen atoms b- electrom collisions strongly depends upon the kinetiv temperature and density of the electrons in the upper layers of the atmosphere. In recent years it has been established by means of raido methods that in the F layer of the ionosphere the kinetic temperature T at night is equal to about 150& and the electron density is approximately ne 2*165. Employing an approximate expression for the cross section of excitation oXygen atom by electron collision and assuming Maxwell distribution for t'e electron velocities and effective thickness of the radiating layer to be equal to 30 km, the aut4or obtains for -::1.43*10 quanta per cze. - the number of quanta of the red line the value N' 7 see. steradian, which agrees with the observed value. The gradual drop in the intensity of luminescence in the course of the night can be 1 c?nse werce of the gradual cooling of the radiating layer, and the variation from nigRt 0 night can be in consequence of the irregualr variations in the temperature.1 Continued: For example, for a decrease of T Prom 1500 to 1300 the quantity N decreases by the same order. Frop the computations it follows also that the kinetic temperature in the F layer cannot exceed 1500 , since in the contrary case the radiation of the red line would be greater than 'the observed radiation. (RZhGeol, No 1-1, 1955) SO: Sum No 884, 9 Apr 1956 s T I 7,G 7 --c- PUP- _T llOT r,;D J -"JOIT~t jo -1-`-M,~ 'c SEIATN. 0.A.. akademik; GAZS, V.F., kand.fiz.-miatem.nauk; PUBL'IM, S.B. Presence of dust and gas in diffuse nebulae. Izv.Kr7D.aatro.'i2. obeer. 12:64-87 154. (MIRA 11-4) Olebula,j) (Interstellar matter) PIULO NER. S. B. USSR, A, t", -c rz; na ."I (7, nil P' ke D P. -~d 1 3 r t) r, z u,- I M, -rac' "r" 3S '.or. Ing a' I type F n'.L)k:!:!" e mn e c ame ra In c omb I na t I on w h one % a e,- yellow fltl-pr. Porm 11 we.-,(-- -j,, sumpt- '. onzi .9 re Tna e c f -1 on the distributIon ol- brlwhtn-~is r inear, rf~"la tAor v-;~ zz f'cun,' betw( bu' a e A ! - tudes --,*- tht~ t-ml3slon n.,id - f general a very complex c,f 'nt-pr'r; 3, dus t exis ts i r, d 1 f f IIE: ed no bu I a - - -: to t, I es 10 references , 4 RuBs Ian ( q 1' n(,e ~ "j '-)) ~ Institution Academy of Sciences USISIT-1, Crimean Astrophysi SubmItted January 4, '16 PIKELIM, SOB. Results of the observation@ of solar corona of June 30. 1954. IZV.Kry'M.astrofig.obeer. 11:111 155. (KIRA 13t4) (Sun--Corona) -'-'-----.777 slid -7- 7 7777 .0 us 0, tic fielcl 6f an-Feb, 195_5 45;;47s 'Ar DYBUMIS rac :o .:su a na SUP eous tali, mm bad- 2: I zo the' -Cr anAst Aclid a10 SOB YJSSR j=D rva- Zr SHAYN, G.A.;PIMINER. B.B.;MSAN(N. R.1. Keazurement of polarization of the Crab nebrulas. Astron.shur. .32 no-3:395-4W 3-0 155- OIMA 9: 1) lArymakaya astrofisicheakaya observatorlya Akadexii nauk SSSR. (Nebulae) (Polarisation (Light)) PIKILIMM, S.D.; GIN33URG, Y.L.; SHKWVSKIT, 1,S. Mechanism of particle acceleration IL envelopes of save* &ad superseve.e. Astroz. zhur. 32 no.6:50-) 513 W-D 155. (Star$, Now) (M72A 9:2) PRELINER. S. -R., GIRS-MG, V. L. and SWLOVSKIY, 1. S. "Radio Radiation of Discrete Sources," a report delivered at the Symposium on Radioaatronoay held at the Jodell-Bank Experimental Radioastronomical Station# Manchester University, Englan, is summarized in the account of this symposium in an article by V. V. VITKEVICH in Vest. Ak. Nauk SM for January 1956. St=. 900, 26 Apr 1956. PIKICLINER, S.B. ?heory of magnetic storms and auroras. Izv.Kryn.astrofiz.obeer. 16:104-121 156. Ma 13:4) (Auroras) (Magnetic storms) PIKE41HER, S.B. Dynamics of diffuse matter. Izv.Kr7m.antrofiz.obser. 16:1,W-14.-7 '56. (JURA 13:4) (Interstellar matter) AMIMM 3 B -S . - - " 0 -to 6AM -- -- Symposium on radio astronomy hold at Jodrell Bank. S.D. Astron.shur. 33 no.lo.114-120 Ja-P 156. (KUU 9: 6) (Jod.roll Bank, Ragland-Radio astrousar-Coagressee) '-I , , PIKIL'MM, S.B. "I' ~ Spiral notion of prominence knots. Astron.shur. 33 no.5:641- 645 S-0 '56. (MLRL 9:12) 1. Krymakaya astrofisicheekaya observatoriya Akademit nauk SSSR. (Sun-Prominence*) PIKELIKER. S.B. - .,-- .-- Ji~~etjb field of the Crab nebula and the central @tar [vith summary in English]. Astron.zhur. 33 no.6:785-799 1~-D 156. (KIaA 10:1) 1.Krymskaya astrofisicheekaya observatoeiya Akademit nauk SSSR. (fiebulae) (Magnetic fields) FIXILIMIR, S.B. doktor fiziko-matematicheskikh nauk. Magnetic field of the Galaxy. Priroda 45 no.12:27-34 D '56. (Magnetic fields) (Kilky way) (MLHA 10:2) PIKELIMM, S.B. Interstellar light polarlsation. Usp.fiz.nw, 58 no.2:2a5-320 F 156. (cosmic rve) (Interstellar matter) (Polorlsation(Idght))(MUL 9:6) PIKSLIMM S.B. G.A.Shain; obituary. Astron.tair,,no.172:1-2 Ag 156. (?U.RA 10:1) (Shain, Grigorli Abramovich. 1892-1956) Name: PIKELINER, Solomon Borlsovich Dissertation: Investigation of the motion and lumineacence of Interstellar gas Degree: Doe Phys-Hath Sol Affiliation: Crimean Astrophysics Observatory, Acad Sol USSR Defense Date, Place: 28 Feb 55, Council of Moscow Order of' Lenin State U imeni Lomonosov Certification Date: 9 Mar 57 Source: BIWO 13/57 AC.t NR, . Am6026m___ Monograph URT-7 Pikel'ner.-SolomDn Borinovich Principles of cosmic electrodynamics (Osn*ovy kosmicheskoy elektrodinamiki) 2d rev. and enI. Moncow, Izd-vo "Nauka", 1966. 1107 p -Illus., biblio. 5000 copies printed. 70PIC TAGS: plasma physics, Plasma wave, plasma stability, plasma interaction, -ovaz= electrodynamics, 6ftiftr,~'_ -;S=~ &qtdr=dP=_rA: ca ==a 04 magnetohydro- dynamics, astrophysics , 006mokci6! PURPOSE AND COVERAGE: This book is intended for the general reader interested In the principles of cosmic electrodynamics and its relationship to astrophysics and geo- physics. Emphasis is on the physical aspects of the problem. Mathematical analysis is kept to a minirmim; it is used only to illustrate a point, and is limited to relatively simple operations. The first several chapters deal with the general properties of plasma, magnetohydrodynamics, wave phenomena in a plasma, and i plasma stability. The subsequent chapters explain various plasma-associated phenomena without going into too inuch detail or mathematical interpretation. There are 331 references, more than half of which are non-Soviet. TABLE OF CONTENTS [abridged]: Card 1/2 UDCe 523,037 ACC NR, Am6o,,>6753 Foreword -- 6 Introduction to the second edition -- 8 Ch. 1. General properties of plasma - 9 Ch. 2. Interaction between a magnetic field and a moving conducting medium 58 Ch. '3- Waves in plasma -- 93 ch. 4. stability -- 14o Ch - Ch. 5. Certain forms of motion of a continuous medium -- 200 6. Magnetohydrodynamics of the galaxy and stars -- 259 Ch. 7. Magnetohydrodynamics of the sun -- 308 Conclusions -- 394 Internation system of units -- 396 398 FM co-,,,~ I . 201 SUBM DATE: igmar66/ ORIG REF- 161/ OTH REP: 170 ACC NR- APM01506 SOURCE CODE: UR/0033/66/043/006/lil-)/1142 AUT11OR: [Avshits, M. A,; Obridko, V, N.; Pikel'ner, S. B. ORG: I ris t i t uL c of Terrr-sLrial Magnettsm, Ionosphere, and Radio~:-tve Propaga' 1111"', AN SSSR (In-L zemnogo magnetizma, ionosfery i rasp ros t raneniya radiovoln A!~ -~,;SR) State Astronomical Institute im. P. K. Shternberg (Goa. BBtronomicheskiy In-,) TITLE: Radio emission and atmospheric structure above sunspots MURCE: Aqtronomicheskly zhurnal, v. 43, no. 6, 1966, 1135-1142 'TOPIC TAGS: radio emission, sunspot, 1,hut(,sphere, chromosphereIA 1 f ve!i C! ;3 1 !corona IABSTRACT: The circularly polarized radio emission on centimeter wave Jettj~lh: front tile iregions above sunspots requires the presence of a magnetic field It 1, 1000 G ind ,)ronal' Memperature a, 106 K. Direct observations of magnetic fields in the photosphore atid jehromosphere as well as theoretical considerations on intense broadening oll I Lube of lines of force in rarefied atmospheric layers show that field strength of 11 '-'- 1000 G is found only at heights not exceeding 3000 km. This implies that tile corona iloparently begins at a small height above spots. A model of a radio source it; computed using the radio spectrum of sources and data on circular polarization. llydroatatic density dis- tribution is assumed. The radio data allow reliable determination of tempvraLulc ('11 1height. The sharp boundaries of the source, its radiation directivity, and Ito coln- Card l/ 2 UDC: 523.746 ACC NR: kP7001506 cidence with umbrae are also explained. The difference betweeti the chlrtnoq):~c~ri, a~,ove !the spot and nor-mil chromosphere is associated with small dissipation of AlIveri and !accelerated waves in a strong field. I'he slow (sound) waves fade in the low (hromo- spheric parts, where they do not cause noticeable heating. Apparently on1v accelerated :waves reach the corona, where they are transformed into other types of waves and fade ;at great heights. From there, the energy is passed by heat conduction to the low ,parts of the corona responsible for radio emission. Orig. art. has: 2 formulaH, 12 figures, and 1 table. I .SUB CODE: 03/ SUBM DATE: 22Mar66/ ORIG REF: 016/ OTH REF: 009 Card 2/-2 A _V" 7.1,TY, PRELIM, S.B. . q, . G.A. Shain (1892-1956). let.-aetron, 1681. no.3:551-607 '57. (Shaln, Grigorti Abramovich. 1892-1956) (MIRA 11:1) ?I!ML'JUQ- Symposium ot radio amtrouonW. Top. koem. 5:279-?82 '57. (Jodrell Bank, Ingland-Radio AstronoNW-Comeresses) (Y,;..rtA -.~ 9) AUTHORs Masevich, A. G. TITLEt The Problem of Cosmic Gasdynamics. In International Conference in the USA. (Problemy kosmicheskoy gazodinamiki. Mezhdunarodnaya konferentsiya v SShA.) 30-11-23/23 PERIODICALt Vestnik AN SSSR, 1957, Vol. 27, Nr 11, pp. 140-143 (USSR) LBSTRAM The physicists# interest ih these problems has constantly in- creased, as the problem of the acceleration of cosmic rays and their lives in the space of the galactic system, as well as the investigation of the formation of interastral magnetic fields is closely coni.ected with the motion of the so-called interastral gases. Representatives of astronomy, physics and mechanics met in Cambridge (Kembridzhe)o UBAI this was the third international symposium devoted to problems of cosmic aerodynamics. The report by the Dutchman Van der Kholst (ob- mervations of the radioemission on the 21 am wave) caused great interest. G. Vokuler (USA) reported on the observationB made in Australia of the spiral structure of the galactic system. 0. Vilson (USA) dealt with the new research data regar- ding the inner kinetics of the planetary nebulae, G. Myunkh Card 1/3 (USA) with the internal motions in the nebula of Orion, The Problem of Cosmic Gaudynamics. 30-11-231/23 R. Minkovskiy (USA) reported on the investigation of the group of fiber-like nebulae in the Swan, R. Devis (England) thoroughly examined the physical conditions in the gas-dust clouds on the basis of the most recent results of the observ- ation of radio-radiation. Much attention in reports and dis- cussio" was paid to the problem of the dissipation of energy. Kh. Petchek (USA), L. Birman and A. Shlyuter (German Federal Republic - FRG) talked on this topic. Some speakers dealt with the nature of the magnetic field of the spiral extensions of the galactic system. Very great attention was paid by the conference to the problem of the gas-corona and of the forma- tion of the radio-radiation (S.B. Pikellner). V.A. Ambartsumyan talked on the genetic connection of-y_o-u-ng___Wtars with the di- ffuse environment. By means of observations made he rejected the hitherto existing assumptions with regard to the formation of the stare from an interastral substance. The members of the sovist delegation made themselves acquainted with the instit- utions and the organization of the optical observations of artificial earth satellites in the USA. The delegation visited the astrophysical observatory in Cambridge (Massachusetts) and Card 2/3 a number of other scientific institutions in the USA. Then the The Problem of Cosmic Gaodynamics. 30-11-23/23 report deals with the details of the optical observations of the artificail earth satellites in the USA. The delegation showed great interest for the nr--nization and equipment of the Numuhusetts Institute of Techpolosy. AVAILABLE: Library of Congress Card 3/3 AUTHORS: Pikel'ner, S. B. and Shklovskiy, 1. S. 497 TITLE: An investigation of the properties and energy dissipation of the galactic halo. (Isaledovaniye svoystv i dissipatsiy energiy gazovoy korony galaktiki). PERIODICAL:"Astronomicheakiy Zhurnaln (Journal of Astronomy), 1957, Vol-54-1 No.2., pp. 145-158 (USSR) ABSTRACT: The distribution of the sources of nonthermal radio- emission of the Galaxy is discussed. The division into a homogeneous sphere and an "Oort-Westerhout" sub-system is artificial. There is some concentration of emission towards the plane and centre of the Galaxy. The strength of the magnetic field,in the upper (Hl','~3-10 t)) and'lower (H-;*6.l0-'j) layers of the halo is estimated from the distribution of radio- emission and two hypotheses: 1) the concentration of cosmic rays is proportional to the field strength, 2) in the upper layers of the halo the magnetic pressure is about the same as the pressure of cosmic rays. The pressure of the magnetic field and cosmic rays at the height z-10 kps is balanced by the weight of the upper layer. Fro% thi condition the density of the layer n> 0.6-10-4 cm-S is estimated. Evidently the gas pressure does not play an essential role in supporting the halo. To keep the cosmic rays the field of the halo must be irregular. Hence the strength. Some examples of halos, with incomplete ionization and in rapid motion, are given. The Large 497 An investigation of the properties and enerry dissipation of the galactic halo. (Cont.) Magellanic Cloud is surrounded by an extenGed n&lo ~ cm-3 having a neutral hydrogen concentration n , 8.1u on the periphery. High velocities did noL lead to great ionization in the nucleus of our Galaxy, eviaently because of the action of the field. Recent radio observations show that the Coma cluster of galaxies is surrounded by a halo, with a radial velocity dispersion - 50u km/sec. The motions are undamped and do not lead to a complete ionization of the gas, because of the magnetic field. Radio observations at low frequencies of galaxies 4enabled the esLimation of n e--,j 0.01 and T - 10 in the lower layers of the halo. 29 references, 11 of which are Russian. Crimean Astrophysical Observatory, Ac. Sc., USSR. State Astronomy Institute imeni P. K. Shternberg. Recd. Dec.11, 1-1L,-). F L AUTHUR: Pikel'ner, S. B. 33-3-2/32 TITLE: Energy dissipation, heating and ionisation of i9terstellar gas by shock waves. (Dissipatsiya energii, nagrev i ionizatsiya udarnymi volnami mezhzvezdnogo gaza). PERIUDICAL: "Astronomicheskiy Zhurnal" (Journal of Astronomy), 1957, Vol.34, No-3, pp-314-327 (U.S.S.R.) ABSTRACT: In a previous paper (1) the author argued that the rare- fied gas in the Galaxy is in the state of rapid motion and fbrMB a spherical sub-system. However, Spitzer (2) has pointed out that at ultrasonic speeds the kinetic energy of the gas is rapidly dissipated into heat. The spherical gas sub-system was discussed in another paper (3) where it was shown that 6the field strengths in_g spherical system are -1 6 x 10 Oersted and -,%,3 x. 10 Oersted in the upper and lower_~ayer~ respectively, the mean gas concentration being 10 4 cm-2. The latter falls off with increasing radius. It was also shown in that paper (3) that the presence of a ma~pietic field whose energy is comparable wita the kinetic energy of the gas should lower the dissipation of enerb-y. atle 3./4 In the present paDer the d-issipation is calculated and estimates are made of the heating and tnermal ionisation of the gas due to magnetohydrody-namic shock waves. 33-3-2/32 Energy dissipation, heati J25 and ionisation of interstellar gas by shock waves. (cont. For simplicity, only perpendicular waves are considered, i.e. waves in which the magnctic lines of force are parallel to the wave front. It is shcwn that if, on the average, the magnetic energy density is equal to the kinetic energy density and is much greater than the thermal energy, then the motion takes place with the velocity of sound and shock waves are very weak. Rext, the effect of cosmic ray pressure is estimated. In the galactic conditions the cosmic ray pressure is of the order of the field pressure. It is shown that the irreversible energy dissipation is given by: q = 0. 044 E iQ - 0. 040 E where the first expression is derived by taking into account the cosmic ray pressure and the second by putting pc.r. = 0; B is the energy of the wave (magnetic + kinetic) per gram. The velocity of motion of the gas, calculated Caxd 2/4 by taking into account the cosmic ray pressure Pe.r. , is subsonic:- cl--%& 1-3v 33-3-2/32 Energy dissipation, heatin and ionisation of interstellar gas by shock waves. (Cont.~ to estimate the temperature of the gas, or the degree of ionisation of hydrogen, from observations, then the calculations carried out in this paper could be used to estimate the magnitude of the energy dissipation and to obtain more accurate values of n and H. In the absence of the field H, & Q and & T will be higher by a factor of 20-30. In this case the first wave ionises the gas by 30 to 4M- and subsequent waves almost complete the ionisation. There is one table and 8 references, 5 of which are Slavic. SUBMITTED: December 11, 195c. ASSOCIATIUN: Crimea Astrophysics Observatory, Ac.of Sciences USSR. (Krymskaya Astrofizicheskaya Ubservatoriya Akademii Nauk SSSR) AVAILABLE: Library, of Congress Card 4/4 1\ F v Toprogy kobsogm14 t. 6 (Problems In Cosmogony. V41. 6) Moscow, Isd-vo AN SSSR, 1958. 367 P. 2,000 copies printed. Sponsoring Agencyt A)r&4a&17a nauk SSU. AstronamIchowdy worst. ARTICLU Flagaltekly. W.A. Ca Uw Origin and fralatIce of ContLemU arA O"ans 5 at,, V.1 latest Data in Determining the aar".8 ute 40 39 &*via, B. To. History of the Mom's Platatice =6 tkw Meologleal Properties at Its Material 6 Safronov v. a. on the orowth or Terrestrial namets ~~)Alfvam. L On the Origin of tkW Solar 37219m R1W A. Ta. wA14%oTlyt. DIslAtegratlem Preseason t ru ati i im n Eli;t d a *swe es Quas n ai v 0 " s M r & * b l" V u SGb: 1~ v ah Ies of Planstary Nebulas . a Oursadyan, O.A. Dynamles of Planetary Nebulas 15T HIMA, I.M. Light Pressure and Uw Dynamic* of namstary Nebulas 211 Agek7an, T.A. Interaction of Stars with Dimas Matter 222 Kaplan, 3. A. Magnetic Gas Dynamics and Prc,&ImW of CoamogM7 238 PArkhomanko, P.O. On the Preservation of Contimammas in the Pormation or ziewate 265 Parkh=�31kD P.O. Determinizz the Location or me -W- P=d*rdMt* Theramwelma M Cl r o um ft"k-OLIP-r, 3-D. On the Tboories of the -WpvMdgrG&%- 269 273 In". 0- TU ft&tD Of Cosmology Today R]LPORT3 MakarkLA, B-V. Conference cc Variable Stare apmas, by ths Hungarian Academy of 3clenceo sma Bold in Budapest an August 23-20 1956 , Tarletaidy. T&. P. ayMoat- cc ftobjew In gimstpa. 333 magnetic Phemomema 3A Conde nVaLas IbOlo o P M C 34 . . w. ocrevense so Nor'n"d star* p V&PQftt90w-VGI1yam1ftvv, S.A. Coaferense an %be rhysiss 3 of Plow" mmudse 354 SUBUI, To. L. Conference at the Committee Co cc 60W Dbvbted to RUXWM the PossIbIlitles at tm = ve man cc Extrawastis Astrononq " Coamc~W 812 ! 3 h, . IC&I Coevers"s 3 4 ~_J_LJ,116 -AUTHDR: Fikellnev, 8,B. TITLE: _ThEsa~sic C~oncep~s of Magnet o-Hydro dynamics .(Osnov-nyye ponyatiya magnito-gicirodinami i) PERIODICAL: Izvestiya Akademii Nauk SSSR, Seriya Geofizicheskaya, 1958, Nr 1, pp.46-53 (USSR) ABSTBACT: This is a review paper giving a brief exposition of the ideas lying at the basis of magneto-hydrodynamics and in particular, the effect of the motion of the medium on the magnetic field and the effect of the field on the medium. The equations of motion of an ion and electron gas are formulated in Eqs.(4) and (5), taking into account inter- actions between them and following Schluter (Ref.1). On the basis of these equations it is shown that if the plasma is dense and the field not very large then the component of the electric field relative to the system moviz4,r with the gas and perpendicular to the magnetic field gives the same current density as in the absence of tLe electric field. If the contrary is the case, then the current in the same direction is very much less and there appears a much stronger current density component perpendicular to both the above electric field e and the magnetic field H Car,l 1/3 However, these are only very special cases. Next, the 11,)- 1 -4/16 The Basic Concepts of Magneto-Hydrodynamics. attenuation of a magnetic field in a hard conductor is considered, following Cowling (Ref.?). An expression for the rate of change of the magnetic field as a function of the velocity of the medium, the magnetic field itself, and the conductivity is derived in the usual way and the signi- ficance of the various terms entering into this equation is discussed. The basic theorem of magneto-hydrodynamics is then formulated in the form: in a fluid with an infinite conductivity (or with a finite conductivity but sufficient- ly large characteristic dimensions), the magnetic flux through any material contour remains constant during motion. A discussion is given of magneto-hydrodynamic waves and it is pointed out that they play a major role in cosmic physics. Above all, they give a simple method of increas- ing the field via the transformation of kinetic energy in- to magnetic energy. Furthermore, they appear to be the way by which energy is transmitted over large distances. By means of these waves, energy is apparently transmitted from sub-photospheric layers to the upper layers on the Sun. There, the energy is transformed into heat and constitutes Card 2/3 one of the main reasons for the high temperature of the 4 -)-i-4/ 1(-) Basic Notiolas in Magneto -Hydrodynamics. chromosphere and the corona. A mention is made of the wc-r1k of Kaplan (Ref.10) and Kipper (Ref.11) who developed tkie theory of turbulence in the magneto-hydrodynamic case. Howeverp these phenomena are very complem and have only been investigated in a first approximation. Somewhat simpler phenomena are those connected with magneto- hydrodynamic shock waves which were considered by Hoffman and Teller (Ref.12) and Helfer (Ref.13). There is 1 figure, 1 table, and 13 references of which 7 are Slavic. SUBMITTED: May 14, 1957. AVAILABLE. Library of Corpress. Card 3/3 PIXEw nu ,"Oov Theory, of the 'equilibrium' origin of elements. Vop.kosm. 6:271-276 158. (MIRA 11:10) (cosmogony) PIKEL11M, S.B.; ?CTIK. L.P. ,an cloudn. Izv. Anisotropy of velocities of interstnilar I; Krym.antro'fiz.obser. 18:198-201 '58. 0141Rh 13:4) (Gases, Interstellar) 3(") Mk'A' I BnOK EXTIDTTATION SOV/3236 Pikellner, Solomon Bori-sovich Fizika mezhzvezdncry aredy (Pt,yBir-z of' the Matter) Moscow, Izd-vo AN SSSR, 1959. 215 p. ('74--ries: Akade-nlya nnW; S53B. Nauchno- populyarnaya. serlya) 12,000 roples printed. Ed.: V.G. Fesenkov, Academician; Ed. of Publishing HcruBe: Yu.1. Yefremov; Tech. Ed.: L.A. Sushkova. PURPOSE: This book is Intended for the general reader interested in astronomy. COVERAGE: This is one of the popular science books devoted to Interstellar matter. It gives background information on the stars and on our galaxy, and explains the various complex processes taking place in Interstellar matter and their relation to the processes In stars. It is concl-aded that interstellar matter is closely associated vith the origin and evolution of the stars. No personalities are mentioned. There are no references. Card I/# / FMLIM, S.B. Genetic relatton of star@ of various subsystems (with summary In Inglish]o Izv,Zrym.astrofts.obser. 21:209-614 159. (MIRA 13:6) (Stars) AU'7'"O'~ 1'ikellner, 3.B., Shklovskiy, I.:;. V 7 - . Ivanov-Kholodnyy, G. S. TITLE: On Possible 1-'echanisms of Emission of Discrete Galactic Ob- jects in the Spectral Region 1225 - 1350 X PERIODICAL: Astronomicheskiy zhurnal,1959,vol 36,Nr 2,pp 264-268 (USSR) ABSTRACTt The authors examine the possibility of explaining the emission of discrete galactic sources, observed in the spectral region 1225 - 1350 A , by usual mechanics. However, this explanation requiresthe assumption that the absolute value of brightness of galactic sources in this spectral region were considerably overestimated. The measurings of the H cc line necessary for the investigation were carried out by R.N. Shefov and V.S. Prokudina in the Zvenigorod station of the Institute for At- mospheric Physics of the Academy of Sciences TISSR. There are 9 references, 3 of which are Soviet, 3 American, and 3 English. SUBMITTED: October '17, 1958 Card 1/1 A ( 7 )4 AUTHOR: P. 30V/56-36-5-37/76 T'.'TLE,- Th,!, 9 ~, --j o Yegrt~ -?.ohydrodynami c Shock Wave in a P&-.fa'ly 1_):Az,,Q Gzx i3truk-~ura magnito-gidrodinamicheskoy -1 -;ai-ncy vo-,%y ionizovannom gaze) PERIODICAL~ ZAW-)h_. teoreticheskoy fizik.111959, V~'._ ~f N7. 7, PP l'-36-154 ~UBSR) ABSTRACT Tha fo.~lowing ?roblem io theorati3ally investigated in the pspsi.- Vn ari only ps-rLlally ionized gas, which is e.sir=ed tc It in a wa&i(itic fi,~'.d, a "piston" is assumed to m,-ve in Ai Is to the H 0 -direction, &r,d that produces a plane wave. Interaction between -ed at,~,ms is assumed to be negligible, and two is And yie~:ti wa,~-es -7her, away 'L-~-)m the 'piston", the magnetohybmdyzxdc onve In the :~Iasma and the orddna.-y one in the neutral gas. If `h,~- f-5-,t ~Tariov.E, ldnda of purtieles have the same j6Tp~~t:8SiO.71 Jn *,h#s plasma is lower than in the th.! pr-_!se:nue of the electrons and (--,f ra~q~r_t_'r, p-eEiaL_-0. In the case of gases having the Card 1/3 s,~xno_ (in 10he, "laboratory system"), the wave front will, The Structure of a Sho-~;- Wave :Ln a SOV/56-36-5-37/76 Ionized Gad ~rev m)ve- Y,,'-th greater speed in tne plasma than in the bellow 100,0000 and 4 the case of 1 -,% I --.ni a ;11ro wheii the free lenft of path of , n 'LOO oi 1000 -.i~jiwya less than theit of the neutral atoins, +hV Stf-Jr,"OL e ~Ii Vio E,~,)~k .Fv(! is invmstigated within the domair mo-i-_ or-,u..3 variation of the parameters. The a~~o(,k wav,- In arach a gas consists of a thir. &arm ac -,n'ini-. ty Lnd. a tranoition zone. Proceeding from the if mcti..)n ir a sys-;am of coordinates that is ,-.ovne_-t,ed vril,~ -Oie fruxrn_ the aut.!ior derives an approximated ~f tne !'o:- tao turaLsltion zone with respect A '-f Kgi `-4). It is found that the charge &k_1..hJ1Ar1 if~,-6cf, axezc's-s ~f,senttal influence upon the gene-r-.1 -,I' mo,.- in, L-.- ~. 'L-L reauoes the Beale. As long the we.,e mev be considared to be steady within the zone of -cran.cj't_or., the ordtr of nialmitude of energy dissipation is indepene-ent cf the degroe of ionization. The author finally t Ya. B, Zel'dc,~ich for 1-ds valuable remarks. There are 4 fimiret, Card 2/3 And 7 -references, 3 of which are 3oviet. The Structure of a Magnetoohydrodynamic Shook 'gave in a SOV/56-36-5-37/76 Partially Ionized Gas ASSOCIATION: Krymakaya aBtrofizicheskaya observatoriya Akademii nauk SSSR (Crimean Astrophysical Observatory of the Academy of Sciences, USSET SUBVITTED: November 30, 1958 Card 3/3 AUTFOR: S. E. T i T !-I--- L-ette- -o th. Ed o- Gz v Sound PERIODICAL: n oy I t,~ o i t., Vc ' i-.' pp -18-17-]F~,'~, (TY--i,) ABSTRACT- -~I( pll op~,.,,,'A-'o -~ o!' :io-ma th-ouf-,h th, y Cow- di , ~d , t~~c ord A rif, to r- ~I lip- !Ty(lr~)dynam-l - T, ,-- ~ - r, .. - - "r 7,~ 1 . " ., . , - - r. - - -:1 '7 , - - Letter to the Editor. Grav!~atlona! 77011 Attenuation of Sound The weakening of the flow is defined b:i the lifting the gas: d (rc-1)I(/-' ---- From this it fol ows that This means "hat w.1thl n the of atmosphere (,L~ z extinct-'on '-s t r,: extinc,fon ,XP(-nent_,a, p_~rt- Ic ipated in t~r~ d -Iscussicn of5 The -,e a-k~ 2 Soviet -efercnces, . ASSCCIATIOY: ~-_'~nean AstrDp-ys 0 b s -a t o ryc Q -7 Ca:-d 4/,, -PIKELIZIERO S.B.v-red. [Third Symposium on Coamical Gas DynamicB; June 24-29, 19571 Tratil sinpozium po tossicheskoi gazodinamike, 25-29 iiunia 1957 gods. Pod red. i a predislovier S.B.Pikellnera. Moskva, Izd-vo inostr. lit-ry.) 1960. 360 p. (MIRA 14:10) 1. Symposium on Cosmical Clan Dynamics, 3d, Cambridge, Mass., 1957. (Astropbysice) (Aerodynamics) PIKUI NER, Solomon Borisvich Physics of the interstellar mediwn. dright-Patturson Air force Ba~~e, Prepared by the Liaison Uffice, Techical Information Center, 1960. 1, 224p. il;us., diagrs., graphs, tables. (MCL**66Vl--I,) Translated from the original Russian: Fizika mezhzvezdnoy sredy. Moscow, 1959. Bibliography: p. 222. 89803 S/169/61/OW/0G3/G2.!/_-22 6 0.? V V/j AGG5/AOG5 Translation from: Referativnyy zhurnal, Geofizika, 1961, No. 3, p. 44, # 3G352 AUTHORS: Dvoryashin, A. S., Pikellner, S. B. TITLE: On the Fine Structure of the Sudden Beg Ing of a Magnetic Storm PERIODICAL: "Izv. Krymsk. astrofiz. observ.", 1960, Vol. 22, pp. 144-149 (English summary) TECT: The momentary decrease in field intensity (pri) preceding the magne- tic perturbation with sudden beginning may be caused by the dynamoeffect connected with the increase of ionization of the lower ionosphere. The compression of the magnetic Earth's field which begins at a distance of about 7 Ro propagates with the speed of a magnetic-hydrodynamic wave. Simultaneously, the energy of the fast particles surrounding the Earth (induction acceleration) increases. These partic- les moving along the lines of force reach the polar regions of Earth and there they increase the ionization. It is possible that the perturbation furthers the permeation of particles into the atmosphere. The increase In energy of particles reaching average latitudes is less. Hence the latitude distribution (pri) is explained. Author's summary Translator's note: This is the full translation of the original Russian abstract. Card 1/1 PIMIMM, S.B. Reviev of "Interstellar gas dynamics" by S.A. Kaplan. Astron. shur. 37 no.3:593-594 My-Je 060. (MIRA 13:6) (Gases, Interstellar) (Kaplan, S.A.) S/033/60/037/cD4/002/012 AUTHOR. Pikellner, S.B. E032/E314 TITLE: Mechanism of Formation of Active Regions in the Pres.nnce of a Magnetic Field PERIODICAL: Astronomicheskiy zhurnal. 1960, Vol. 37, No. It, pp. 616 - 621 TEXT: In order to explain the presence of plages. floccull and r.oronal rays, it must be assumed that the presence of a weak magnetic field can lead to the amplification of motion in upper layers of the convective zone. Since the convective currentq have a large Reynolds number, they should be unstable and givi~ rj~, to turbulence. Usually, the velocity of major turbulent pulqatici, is of the order of 100,'v of the velocity of the main stream., Fcr large Reynolds numbers, turbulent viscosity is much greater than molecular viscosity and determines dissipative forces. The appearance of convection '24determined by the Rayleigh number given by; 9P R - (V T V T) Card 1/4 X~ ad S/033/60/03 704/002/012 %31~EAII Mechanism of Formation of Active eg o s in the Presence of a Magnetic Field where g is the acceleration due to gravity, is the volume expansion coefficient which. for a ga-s is equal to T_ 1 . is the thickness of the layer, if it is thin or comparable with the height of a uniform atmosphere )L is the temperature diffusivity, and NJ is the kinematic viscosity. Convection will take place if R > 0 If the numbf-r R~/,~ is large, say. of the order of 10 then stationarv convection is unstable, the motion is unordered and cells ar(- net formed. For lower values of this number, non-stationary conve-c-11"il takes place, i.e. cells are formed but are irregular. Solor granulation resembles this type of convection. It would theref-)rc appear that R XAJ is not too high. However, a simple estimat(- shows that R -%~ 10 10 and, moreover, e. C onv e:V Card 2/4 S/033/60/037,604/002/012 EO~2~E~11 Mechanism of Formation of Active e i ns in the Presence of a Magnetic Field 12-' cells should not be formed on the SUp at all, Schwarzschild (Ref.13) has pointed out that this contradiction can be avoided by using N) turb instead of V. The former is larger by several orders of magnitude and hence R is relatively low. Moreover, X is only slightly greater than \j turb ' " that if convection is present it must be quasi-stationary. Thus, the velocity of convective motions is determined by the equilibrium between the upward forces and the turbulent viscosity force. if the viscosity is reduced, the upward velocity should increase. The intensity of a weak magnetic field is not sufficient to have an effect on the convective stream but may influence turbulence., A few tens of Oe should be sufficient for this mechanism to takc- place. It is argued that any field, independently of its origin and character, should give rise to active regions whose properties depend only on the field strength. In particular, a weak field tends to decrease dissipation and increase convective velocity Card 3/4 S/033/6o/037,4o4/002/012 E03fi/E314 Mechanism of Formation of Active egions in the Presence of a Magnetic Field since, as mentioned above. it does not affect the main stream but damps turbulence This is illustrated by polar plages which are closely connected with the Sun-s -)olar magnetic field The low value of the latter field is the reason for their low brightness and the great depth of the upper boundary, Heating due to polar plages gives rise to polar coronal rays and possiblv the permament solar wind. Complicated spectral variations in magnetic stars may also be related to the influence of the magnetic field on convection. There are aO references 5 English 6 German. I Swedish and 8 Soviet. ASSOCIATIONi Gos, astronomicheskiy in5titut im P,K Shternber 'ga (State Astronomical Institute SUBMITTED. Aptil 10. 196o Catd Li/4 PIKELINER, Solomon BorisovichiKULIKOV, G., red.; LUIUCOVA, L., tekhn. rea. -- [The aun) Solntse. Moskva, Gos.izd-vo fiziko-matem.lit-zT, 1961. 82 p. (Popullarnye lektsii po astronomii, no.11) (MIRA 15:1) (Sun) PHASE I BOOK EXPLOTTATION SOV/5732 Pikellner, Solomon Borisovich Osnovy kosmicheskoy elektrodinawiki (Principles of Cosmic Electro- dynamics) Moscow, Fizmatgiz, 1961. 295 P. 5POOO copies printed. Ed.: B. Ye. Gellfgat; Tech. Ed.: L. Yu. Plakshe. PURPOSE: This book Is intended for nonspecialists interested in cosmic electrodynamics. COVERAGE: The book is an attempt to present in a systematic and simple form the fundamentals of cosmic electrodynamics and their connection with astro- and geophysics. The main emphasis is on physical rather than on mathematical concepts. 'The author thanka D. A. Frank-Kamenetskiy and S. I. Syrovatskiy for their advice, A. B. Severnyy for his photographs of solar formations, and B. N. Gershmar. and R. Z. Sagdeyev. There are 258 references: 135 Soviet, 95 English, 14 German, 7 Swedish, 2 French, and 5 other. Card-1/_4 89319 S/033/61/038/001/002/019 7 3 2-6, // Z 7.,// 2.17) E032/E314 AUTHOR: Pikellner, S.B. TITLE; Th`eiff7elt ;fcl~lml --Rays on the Character of the Magnetic Field and the Formation of Filaments in the Envelopes of Supernovae PERIODICAL: Astronomicheskiy zhurnal, 1961, Vol. 38, No. 1. PP. 21 - 27 TEXT: In the plane of the Galaxy the cosmic-ray and magnetic- field energy densities are roughly equal. 1.S. Shklovskiy has frequently pointed out that this cannot be accidental it is possible that this is connected with the retention of cosmic rays. Radio data show that magnetic fields and cosmic rays are also present in the galactic corona but the intensity of the radio emission gives only the retktion between them. The quantity KH 1.8 is roughly 20-30 times smaller the"disc" (K is proportional to the concentration particles or their energy). in a previous paper (Ref. present author and Shklovskiy assumed that both K decrease so that the energy balance is preserved. Card 1/8 than in of the 5) the and H Kahn and 89319 S/033/61/038/001/002/019 E032/E314 The Effect of Cosmic Rays on the Character of the Magnetic Field and the Formation of Filaments in the Envelopes of Supernovae Woltjer (Ref, 6) assumed that since the distribution of cosmic rays it, a closed stationary system should be uniform, only H decreases. In that case, the particle energy should be 5-10 times greater than the magnetic energy. Hoyle (Ref. 7), on the other hand, considers that the cosmic-ray energy is several times greater than the magnetic energy. The problem therefore arises as to whether the retention of the cosmic raysis possible. The present author argues that the magnetic energy should be comparable with or greater than the cosmic-, ray energy. Moreover, magnetic forces should be comparable with the cosmic-ray pressure gradient and hence the field cannot be force-free in the entire region if the cosmic-ray energy is comparable with the magnetic energy. The equilibrium of' gas in gravitational and magnetic fields is described by~ Card 2/8 ~93i~ S/033/61/038/ool/oo2/oig E032/E314 The Effect of Cosmic Pays on the Character of the Magnetic Field and the Formation of Filaments in the Envelopes of Supcrnovae (!g + 7 P + V p+rot H x H - 0 (1) I k 41r where p is the pressure of the gas Pk is the cosmic-ray pressure, 9 is the acceleration due to gravity, H is the magnetic field and indicates that the gas is subjected to the component of the gradient which is perpendicular to H . The problem is therefore reduced to the investigation of the stability of this equilibrium for P < Pk and H2"Ti< Pk - If the system is stationary and cosmic rays are retained by it, their density should remain constant. Card 3/8 89319 S/033/61/038/001/002/019 E032/E314 The Effect of Cosmic Rays on the Character of' the Magnetic Field and the Formation of Filaments in the Envelopes of Supernovae In this case V p k = 0 inside the system but at the boundary the gradient increases considerably. However, the Galaxy is hardly a closed system with sharply defined boundaries. Ginzburg and Syrovatskiy (Ref. 8) have shown that the chemical composition of cosmic rays and some of their other properties can only be explained if it is assumed that the particles do not return to the plane of the Galaxy from its boundaries, i.e. that they gradually diffuse in the outward direction. In this process, the particle density gradually decreases and ~7pk / 0 inside the galactic corona. More- over this result suggests that the field inside the Galaxy is not quasiregular and curving only at the boundaries since otherwise the particles could easily be reflected back into the galactic plane, If the cosmic-ray density decreases Card 4/8 `9319 S/033/61/038/ool/oo2/oi9 E032/E3i4 The Effect of Cosmic Rays on the Character of the Magnetic Field and the Formation of Filaments in the Envelopes of Supernovae gradually within the corona, then the equilibrium of the gas is only possible if the lines of force are sufficiently rigid so that the magnetic force (last term in Eq. 1) should not be smaller than 7p k * This defines a lower limit for the field strength and means that the field cannot be force free in the region where the cosmic-ray density is not constant. Inside a closed system the cosmic-ray pressure should be constant but should decrease within the limits of' a thin transition layer, In order to retain the cosmic rays a large force concentrated in this layer and directed inwardly is necessary, If the magnetic energy is smaller than the cosmic-ray energy then even in the case where the magnetic force is concentrated in the transition layer it cannot balance the particle pressure and the latter will penetrate the layer in the outward direction. As a result, the system will cease to be stationary and closed, Card 5/8 89319 S/033/bl/036/001/OU2/019 E032/E314 The Effect of Cosmic Rays on the Character of the Magnetic Field and the Formation of' Filaments in the Envelopes of Supernovae the cosmic-ray density gradient will appear and the instabilitv will be propagated in the inward direction, Even when the magnetic energy and the particle energy are equal, the transition layer will only be able to retain the cosmic rays when the magnetic force is comparable with the pressure gradient. A force-free field within a closed system should give rise to surface currents responsible for the discontinui~v in the tangential component of the magnetic field, These currents cannot compensate the pressure due to relativistic particles since for these particles the magnetic force is also equal to zero. A single force-free field of the type described by Woltjer (Ref. 11) for the Crab nebula would be unable to retain the cosmic rays in the nebula. Retention of the cosmic rays is only possible because the filaments are massive formations capable of withstanding the pressure upon them, Thus the cosmic-ray density in the galactic --orona cannot6Y constant because tiiis wou Id Icad to instabi lity Car S/033/bi/o38/ool/002/019 E032/E314 The Effect of Cosmic Rays on the Character of the Magnetic Field and the Formation of Filaments in the Envelopes of Supernovae at the boundary where all of' the cosmic-ray pressure gradients would then be concentrated. Since a cosmic-ray pressure gradient should exist insiae the corona,the field in that region cannot be force-free and quasiregular. In the envelopes of supernovae the cosmic rays are enclosed and their pressure gradient at the boundary is large, The main mass of theawelopeis also concentrated at the periphery and if a tangential field is present a peculiar type of instability is produced, in which the field is forced out by cosmic-ray pressure in the form of isolated loops and the gas is ejected by the accelerating field along the lines of force and forms filamets. The curvature of the arcs formed by the lines of force between the filaments suggests that the magnetic and cosmic-ray energies are roughly equal, In principle, the cosmic-ray pressure can be determined from the condition that it is equal to the pressure in Card 7/8 89319 S/033/61/038/001/OU2/019 E032/E314 The Effect of Cosmic Rays on the Character of the Magnetic Field and the Formation of Filaments in the Envelopes of Supernovae interstellar gas condensations which are envelope. Such condensations have been in Lassiopeia. However, a detailed calculation become possible when photometric data on available, There are 14 references: 5 9 non-Soviet. observed within the found in the source will only the spectrum become Soviet and ASSOCIATION: Goa. astronomicheskiy institut imeni P.K. Shternberga (State Astronomical Institute imeni P.K. Shternberg) SUBMITTED: September 17, 1960 Card 8/8 1.!3.; pa~Ll: 'I" j.". -- On ',.' c--l- I- article c,: - clio Lci.:-c :..I' J G: . ' :* 3j c.- 1 1, - - "11. " z a. r E .~ . i:JC,6-11 [ Ja-7 Ia. ( 7. 1 (;Lltr(.Ilc,!:Y) - PIKELINER., S.B, Formation of corowd condenoations a+e active regiona. Astron.zhur. 38 no*3:552-553 MY-Je 1619 (VM 14:6) 1. Gooudaretvennyy astronomicheskiy institut imeni F.K.Shternberga. (BuD--Corona) V,71L'NIKOV, O.A.; UHL'NER, S.B. "Course of Practical -strophysics" f~y D.1A.Fart *ynov. Rpviewed ~'v O.A.Me.Vnikov, S.B.Pikel'ner. Astron.zhur. 3P no.5:10(14-1Vr( S-0 (I. (MIRA 14:9) (Astrophysics) (Martynov, D. IA.) PIKELINER, S.B.; KOGANS V.I. OPhysical processes inside stamm by D.A.Frank-xamenatilkii. Reviewed by S.B.Pikellner, V.I.Xogan. Uap.fia.naak ?4 no.1:181-18.4 iV o61. :. (KERA 14:6) (Astrophysics) (Frank-Kamenstskii., D.A.) 0 42 %1523/090/0 .3/00.5/0 S/03 VUZ/03 9/006/00't /0~-' 't AUTHOR: Pikc-llner, S.B. TITLE i Formation of a chrOITIOSP110riC net,~ork i,i,i tho of the in.ignetic field PERIODICAL: Astronantichesitty zhiirnn I , v. 19, no.h, 1962, ~7-)-)70 TEXT: A model is con.-,idered in which it is fibsmaod, for th, sake of simplicity, that the lines of force passinS tht-oil.,;h a section of the siirface are vertical. It is further supposed t1i it there are two Inyers of convective cells. The upT)er layer ~;iv(- rise to granulation nno the lowor one contains motioi)m energy i- appreciably higher than the field energy so t;iot t;1- lo-- er layers deforming the lines of force, may be ignoreu. Ti.- ,i- velocities in the cells are directed from the centre tt~ th~ (1-1~1-~' fortaing close lines passing thr~jugh the lower parts of the c(-1 Is. In this way tlv~ gas flows townrds the networl-, formt-(i 1j'. tliv boundaries of thr, convective cells. This gives rise to a displacement of the linen of force so that their number pcr unit area becomes greater at tho!se boundaries. This "condensat ion" of lines of force is transmitted in t)i-- forin of dynamic waves into the upper layer itntl then to thf- photo, Card 1/2 Formation of a chrot-riospheric 5/033/6 2/0!q/0o6/o(, If /o-,'i r, 0 -12 /r 1. 4 chromosphere aii(I cor,ina. The arts aL~,) )rop;ii;atf_-(; it, -t clownward direction -!wre t!ie ilvdi-o'lVililmit -Ire tile magnetic forces so tiiat tiic 1:tttvr do ni)t dotf-rriiiiie f!i- i. Judging fro.n the tiiitj of exist(~iice t)f f,i(. fiett-ork, t,1)(' (:!-.,ft -r- istic time of oxistr ice of a cell 14 'Ibollt 2"1 11WIt'.4. Diii-i ; i i i time tile gas i il a pa r t i cu I ik r c f, I I c twip I o t o.-3 a s i;ip, L v c y cI o ( revolu t i on ) a rid is w-w c P I 1 1) 111.,4 t,, fo riii i n (J v r) -n,: nii tI y' It:w ori~jtial cell (,ion-st.-,tic) iory wivi-c t toji) . Tit(, litiefo; ol ,,. c then redistrio.-te thei;tselve!, ag:iin into ri new net-oj-%. I t I that tile I)er:L,i(; if Cie w.ives prop.-ivatirig iii tho . I ""( I Is aboij t ;iwi i - . I',t1:111Y)CWl CIMVPC tit-11-1 IV-4 1-1.14V t-) .1 !1 1 1.1 in chromospheric ettii.4 iion and fiv,i( e tit(, notwork (_ovt,rii- tit, surface of tit(, un accurrli,ice witli thf- ibokv I!, -11su observed in Call ancl If Cx lines. rh e pro!.; Pric P C C. S ')!I tile entire solar sur!.-cc i7l (jicatvs tilat .. wealk M.1trietic I'l (.11 1 i present everywiiere. ASSOCIATION: G0.9 . a S t ronomi chesk i V i 11.9 t i tit t im . p Sit t p (State %Str-')?101T11c.1I lrititiite Iiiii-ni 11.1%. Slit -tw- r,~ SUAMITTED t ff , V 0 , 1 90 Card 2/2 PIKELINER, S.B. Okerodynamic pbenomena in stellar Atmospheres; proceedings of the Fourth SympcAium on Cosmical Gas Dynamics, Bologna, 196108 Reviewed by S,B. Pikellner. Astron zhur. 39 no.6:IIJ&-IIAI N-D 162. IMIRA 15:1-1) (Stars--Atmosphere) ~A036547 BM EXPLOITATION a/ Kaplan, Savull Aronovich; Pikellner, Aft'low Awlauu. Interstellar mediva (Mezhzvezftaya sreda),, Moscow, Fismstgiz, 1963v 531 P. illus., biblio. Errata slip inserted. 3,50D copies printed, TOPIC TAGSt Interstellar medium, interstellar g",,-interstellar bydrogen,, interstellar dust, interstellar magnetic field, Interstellar gas dynavics, galactic evolution, radio transadesion TABLE OF CORMTS [abridgedli Foreword 9 Ch. 1. Interstellar hydrogen - n 'Ch. Il. Physical state of Interstellar gas - 105 Ch. Ill. Interstellar dust - 191 Ch. IV. Interstellar magnetic fields and radio transmission - 277 Ch. V. Interstellar gas dynmioa and evolution of the Interstellar sedium - '1072 Appendices - 480 Bibliography - 510 cod 2./2 AN4036547 -SUB ODIZI No AS 281 LoctO SUMTM ACQS 06Ayr& MR JW 3DVI PIKELINERV S.B.; GINTSBURG, M.A. Mechanism of type-2 bursts of Bolar radio emission. Astron. zhur. 40 no.5t842-846 S-0 163. (KRA 16:11) 1. Gosudarstvennyy aBtronomfbht*kiy institut im. P.K. Shternberga i Institut zemnogo magnetizma, ionosfery i radio AN SSSR. KAPLAN, Samuil Aronovich; PIKELINER Solomon Borisovich; =4 - Zl------,--, - - AMBARTM-TYAN, V-.A., red.; KffSTELI , E..T1. Fea. ~ S-Vm"~-Y' .9 p A.B., red.; SOBOLEV, V.V., red.; i7~LlKcy, G.S., red.; AKSELIAOD, I.Sh., tekhn. red. [Interstellar medium] Mezhzvezdnaia sreda. Moskva, Fiz- matgiz, 1963. 531 p. (MIRA 17:2) ACCESSION NR: AT4019685 S/2555/63/009/000/0060/0069 AUTHOR: Pikellner,S. a. TITLE: The diffuse medium and formation of stars and stellar systems SOURCE: AN SSSR. Astronomicheskiy sovet. Voprosy* kosmogonil (Problems of cosmogony), v. 9, 1963, 60-69 TOPIC TAGS: astronomy, astrophysics, stellar system, diffuse medium, star, star formation. hyperon star, cometary nebula, globule, galaxy ABSTRACT: Arguments in favor of the origin of stars from gas are given. Gravita- tional condensation of systems of different orders is considered. The paper be- gins with a refutation of the Ambartsumyan hypothesis that stars are not formed from. diffuse matter, but from dense bodies of an unknown nature, possibly hyperon stars. The hypothesis that stars originate from globules is explored next and it is noted that cometary nebulae are an indirect confirmation of the validity of this theory. The evolution of a compressing mass, real time of compression and inter- mediate and extreme cases of compression are considered. The Importance of taking .rotational and magnetic fields into account when computing gravitational compres- sion is stressed. Star formation must be considered as occurring in large groups .r..plusters,oot in an individual group of cluster; this viewpoint is emphasized. Card 2 ACCESSION NA: AT4019685 The breakdown of spherical clusters into a great many stars Is important because the formation of stars in spherical clusters is occurring at the present time. The final problem considered Is the fact that star formation Is still continuing in spiral and irregular galaxies but already has virtually.ended in elliptical galaxies. Orig. art. has: 2 formulas. ASSOCIATION: ASTRONOMICHESKlY SOVET AN SSSR (Astronomical Council AN =R) SUBMITTED: OOOct62 SUB CODE: AS DATE ACQ: 12Mar64 NO REF SOV: 009 ENCL: 00 OTHER: 008 2/2 Card PIKELINER, S.B. Anallsis of possible mechanisms of the formation of magnetic fields in radio sources. Astron.zhur. 40 no.4:601-611 Jl-Ag '63. (MIRA 16:8) 1. Gosudarstvennyy astronomicheskiy institut im. P.K.Shternberga. (Magnetic fields (Cosmic physics)) (Radio astronomy)