VbvAstE-001

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to the limit (11.19). As result, a searching of ≪black hole≫ inside stellar objects of our Galaxy seems as hopeless. On the other hand, stellar objects, consisting of hot relativistic plasma - a quasars, in accordance with their mass and density, may stay ≪black holes≫. The process of collapse is not needed for their creation. As the quasar mass M qu ≫ M Ch , all other stellar objects must organize their moving around it and one can suppose that a ≪black hole≫ can exist at the center of our Galaxy. 93
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Boris V.Vasiliev ASTROPHYSICS and a
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4
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5 The main parameters of star 29 5.
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8
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theories of stars that are not purs
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But plasma is an electrically polar
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can be described by definite ration
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But even at so high temperatures, a
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2.2 The energy-preferable state of
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20
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3.2 The equilibrium of a nucleus in
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24
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As a result, the electric force app
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and in accordance with Eq.(4.11), t
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The total kinetic energy of plasma
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we obtain η = 20 = 6.67, (5.24) 3
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40 N 35 30 10 9 8 7 6 5 4 3 2 1 A/Z
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One can show it easily, that in thi
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2.10 log (TR/R o T o ) 1.55 1.00 me
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averaged temperature and averaged p
Page 43 and 44: log R/R o 1.5 1.3 1.1 0.9 measured
Page 45 and 46: The Table(6.2). The relations of ma
Page 47 and 48: The Table(6.2)(continuation). N Sta
Page 49 and 50: The Table(6.2)(continuation). N Sta
Page 51 and 52: log T/T o 1.0 0.9 0.8 0.7 0.6 measu
Page 53 and 54: Figure 6.4: The schematic of the st
Page 55 and 56: 54
Page 57 and 58: Simultaneously, the torque of a bal
Page 59 and 60: At taking into account above obtain
Page 61 and 62: 60
Page 63 and 64: of periastron rotation of close bin
Page 65 and 66: 8.3 The angular velocity of the aps
Page 67 and 68: N -3.0 -2.5 -2.0 -1.5 -1.0 -0.5 0.0
Page 69 and 70: Figure 9.1: (a) The power spectrum
Page 71 and 72: Figure 9.2: (a) The measured power
Page 73 and 74: 9.3 The basic elastic oscillation o
Page 75 and 76: 9.5 The spectrum of solar core osci
Page 77 and 78: star mass spectrum. At first, we ca
Page 79 and 80: where ˜ λ C = m ec is the Compto
Page 81 and 82: This energy is many orders of magni
Page 83 and 84: 82
Page 85 and 86: Figure 11.1: The steady states of s
Page 87 and 88: It opens a way to estimate the mass
Page 89 and 90: N 10 9 8 7 6 5 4 3 2 1 0 1.0 1.1 1.
Page 91 and 92: This makes it possible to estimate
Page 93: to p F ≈ mc, its energy and press
Page 97 and 98: approach to the separation of the E
Page 99 and 100: is evident as soon as in this proce
Page 101 and 102: Figure 12.1: The dependence of the
Page 103 and 104: Figure 12.2: a) The external radius
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Page 107 and 108: It gives a possibility to conclude
Page 109 and 110: This allows us to explain the obser
Page 111 and 112: [14] Landau L.D. and Lifshits E.M.:
Page 113 and 114: N Name of star U P M 1 /M ⊙ M 2 /
Page 115 and 116: [9] Gemenez A. and Clausen J.V., Fo
Page 117 and 118: [30] Hill G. and Holmgern D.E. Stud
Page 119 and 120: [52] Semeniuk I. Apsidal motion in
Page 121: [75] Andersen J. and Gimenes A. Abs
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