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Content 1.0.0. Introduction 2.0.0. Setup of the problem 3.0.0. Resolve of the problem 4.0.0. Investigation of the result Connection with the Classic Law of Hydrostatic Balance 5.0.0. Integral mode of the result Investigations of the result in integral mode 6.0.0. Conclusions 7.0.0. Energy of the gravitational bodies 8.0.0. Appendices 8.1.0. Abbreviations 8.2.0. Useful Sites 9.0.0. Bibliography 1.0.0. Introduction In the space are seen a row massive bodies - stars, planets, big satellites. They posses following features: - Their form is spherical in first approximation. - Their real form is of the kind of the fluid, rotating in field with central symmetry. - Their structure is laminated. - They posses theirs own source of the energy/heat, which is growing with mass of the bodies in most cases. Today in the studying of these objects, the Law of Hydrostatic Balance /LHB/ is used, and it is written in many forms depending from the level and the aim of the particular investigation. This law is checked on the Earth surface and it is unconditionally right. In this case, and in the frames of the technical goals, the gravitational field has plane-parallel symmetry. In the general case gravitational fields have centripetal/central symmetry. This presupposes availability of the General Law of Hydrostatic Balance /GLHB/, which is rendering of account the central symmetry of the gravitational fields, and which in its boundary approximation towards body's surface reaches the form of the Classic law of Hydrostatic Balance /CLHB/. The finding of such law is the aim of this work/attempt. 2.0.0. Setup of the problem. 2.1.0. Let's examine the following physics object: Spherical body with volume , consisting of layers, limited by concentric surfaces with radii respectively of the above limit, and of the lower limit. Every layer is with its own volume , and is consisting of elements with density - constant for the layer. Elements are in compact packing - i.e. in the layer have not empty rooms/caverns. Interaction between elements is only gravitational. All rest interactions are set at naught. Have not outside influence. Every element is gravitating and is giving its contribution into the common field of the corresponding layer , and into the full field of the body. In the same time it is feeling gravitational impact from the other elements of the body, which integral expression is the weight of this element. Gravitational interaction is describing by the Newton's law and it's consequences. The sum of the weights of the elements /in the frames of the layer/ will give the weight of the full layer . The sum of the all layers, laying over spherical surface with radius and area will form the stress over this surface. The ratio will form the pressure over this surface. Let's find . 2.2.0. Draft and brief writing. Fig. 1 where: - Mass of the spherical laminated body - Outer radius of the body - Arbitrary layer - Mas of the sphere with radius - Radius of the upper limit of the layer - Radius of the under limit of the layer - mass element of the layer - distance from the body's center of the - Density of the element , respectively of the layer - Average density in the sphere with radius - mass of the part of the layer between spheres with radii and - Gravitational constant The goals: Weight of the element Weight of the layer Stress and pressure over under limit of the layer Considerations will be done in spherical coordinates. Back to Content 3.0.0. Resolve of the problem The weight is the sum of two components and caused by attraction of the masses and over : Let's express : spherical coordinates in the frames of the layer and See Appendix 1 This expression has a sense only in the case , which is reality for the bodies investigated with seismic. The weight of the full layer will be: The proposed integral is trivial, and its result is: See Appendix 2 The layer was chosen in random way (arbitrarily). The same kind will be the expression of the weight for the every another layer . All layers, from most outer to the layer including, lay over under limit of the layer . Consequently, the sum of the weights of all layers above , and it including, will form the stress over the surface upon consideration. The pressure over under limit of the layer will be: And finally: This is the basic result for our goals Back to Content 4.0.0. Investigations of the result. Connection with Law of Hydrostatic Balance. 4.1.0. Checking with dimensions Obtained result possesses dimension of the pressure. 4.2.0. Boundary behavior toward See Appendix 3 When every another , laying between and , will tend to . Thus expression in the small brackets will nullify, and with them the full sum will nullify, too. 4.2.1. Let's examine one particular case: The pressure over surface with radius : In this case: Where: is the surface density of the body is the average density of the body What behavior reaches this equation when the layer is very thin - e.g. ? Let's see: . . . . . . 0 In this particular case the pressure incline to , too. But in before boundary case, when , but still , the expression reaches mode known like Law of Hydrostatic Balance - LHB. That means, the formula encloses into it LHB like its boundary approximation. 4.3.0.Boundary behavior toward See Appendix 4 Here is the big difference between new expression and known law! 4.4.0. The case of homogeneous body See Appendix 5 where: Back to Content 5.0.0. Integral mode of the result. Investigations of the result in integral mode Let' examine the case, when the body is consisting from unlimited number very thin layers. In this case: See Appendix 6 All investigations, made in 4.0.0. should be repeated here. The result is the same. Back to Content 6.0.0. Conclusions Formulas are generalizations of the LHB. They are expressions of the central-symmetry force fields. The LHB is boundary case /asymptote/ of the above formulas. It is expression of the plane-parallel force fields. The LHB is permissible only in the case . This is anthropomorphic experience of the human beings. Fluidity is a condition of the substance in which gravitational interaction is dominating. Back to Content 7.0.0. Energy of the gravitational bodies After integration the pressure field, over full volume of the body, should be found gravitational energy of the body. Integration of the over volume of the proposed body gives result: See appendix 7 For a homogeneous body: This formula combined with Principle of Dirichlet gives a physics basis for the bodies expanding. In Appendix 7.2, I have resolved the case only for the homogeneous body. But: - For the most bodies gravitational energy is dominating. - Gravitational force is conservative The distribution of the density along the radius should change distribution of the energy along the radius. Full energy of particular body is one and the same scalar. Back to Content Nikolay Borislavov Kitov nikolakitov@gmail.com 8.0.0. Appendices Appendix 1: Weight of the element from arbitrary layer spherical coordinates in the frames of the layer , Back to main text Appendix 2: Integral for the weight of the single layer Back to main text Appendix 3: Boundary behavior toward Back to main text Appendix 4: Boundary behavior toward For particular , the sum represents real positive number. Back to main text Appendix 5: The case of homogeneous body For a homogeneous body it is no matter how it will be divided by layers. Consequently should play role of the running coordinate. Back to main text Appendix 6: Transition toward integral mode of the result 1. 2. 3. All articles with are omitted. Here should play role of the running coordinate . Back to main text Appendix 7: Expressions for the gravitational energy. 7.1 General case The integration over and is as the same as in the Appendix 2 . Back to main text 7.2 Case of the homogeneous body Back to main text Abbreviations LHB - Law of Hydrostatic Balance CLHB - Classic Law of Hydrostatic Balance GLHB - General Law of Hydrostatic Balance Useful Sites About Law of Hydrostatic Balance - definitions and applying: - Hydrostatic equilibrium or hydrostatic balance - What is a star? - Bullen and Earth's models - Standard Earth Model - Why the earth's core is hollow - the standard earth model Back to Content Bibliography "The Quiet Sun" Edward G. Gibson Manned Spacecraft Center, Houston, Texas 1977 "The New View of The Earth (Moving Continents and Moving Oceans) Seiya Uyeda , W. H. Freeman and Company , San Francisco 1980 "Physique et Dinamique Planetaires" Paul Melchior Louven/Bruxelles Vander-Editeur 1975 "Таблицы физических величин" под редакцией академика Кикоина Москва, Атомиздат, 1976 "Звезды - их Рождение, Жизнь, Смерть" И. С. Шкловский Москва, Наука 1975 "Сверхновые Звезды" И. С. Шкловский Москва, Наука, 1976 Back to Content Nikolay Borislavov Kitov nikolakitov@gmail.com

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posted: | 11/17/2012 |

language: | English |

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Investigation of the behavior of the pressure in the lenths of all radius of the massive gravitational bodies.

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