Newtonian Gravitation of Matter and Antimatter

Similar documents
COMPUTATIONAL THERMODYNAMICS

Introduction to Cosmology

General relativity and the Einstein equations

Black Holes. Jan Gutowski. King s College London

Galaxies 626. Lecture 3: From the CMBR to the first star

The Time Arrow of Spacetime Geometry

General Relativity Lecture 20

General Relativity. Einstein s Theory of Gravitation. March R. H. Gowdy (VCU) General Relativity 03/06 1 / 26

Dark Matter and Energy

Rational derivation of the Boussinesq approximation

Cosmology (Cont.) Lecture 19

General Relativity and Cosmology. The End of Absolute Space Cosmological Principle Black Holes CBMR and Big Bang

Astr 2320 Tues. May 2, 2017 Today s Topics Chapter 23: Cosmology: The Big Bang and Beyond Introduction Newtonian Cosmology Solutions to Einstein s

Arvind Borde / MTH 675, Unit 20: Cosmology

These two lengths become equal when m is the Planck mass. And when this happens, they both equal the Planck length!

AA210A Fundamentals of Compressible Flow. Chapter 1 - Introduction to fluid flow

0.2. CONSERVATION LAW FOR FLUID 9

DARK HEAT. By Kadir Aydoğdu student from MIDDLE EAST TECHNICAL UNIVERSITY DEPARTMENT OF PHYSICS

Numerical methods for the Navier- Stokes equations

The Cosmological Principle

Astronomy, Astrophysics, and Cosmology

1. De Sitter Space. (b) Show that the line element for a positively curved FRW model (k = +1) with only vacuum energy (P = ) is

FXA ρ 0 = 3(H 0 ) 2. UNIT G485 Module Universe Evolution. Candidates should be able to : age of the universe 1/H 0

Relativity, Gravitation, and Cosmology

New Blackhole Theorem and its Applications to Cosmology and Astrophysics

Crossing the Event Horizon Presented by Nassim Haramein

The Definition of Density in General Relativity

Lecture 05. Cosmology. Part I

Physics 133: Extragalactic Astronomy and Cosmology

COSMOLOGY The Origin and Evolution of Cosmic Structure

Gravitational collapse and the vacuum energy

A873: Cosmology Course Notes. II. General Relativity

Quantum Gravity and Einstein s Relativistic Kinetic Energy Formula

Cosmology: An Introduction. Eung Jin Chun

Chapter 1. Introduction to Nonlinear Space Plasma Physics

Outline. Covers chapter 2 + half of chapter 3 in Ryden

2.1 Basics of the Relativistic Cosmology: Global Geometry and the Dynamics of the Universe Part I

The Hopf equation. The Hopf equation A toy model of fluid mechanics

A5682: Introduction to Cosmology Course Notes. 2. General Relativity

Equations of motion from the Minkowski metric.

Numerical Heat and Mass Transfer

The Standard Big Bang What it is: Theory that the universe as we know it began billion years ago. (Latest estimate: 13:82 ± 0:05 billion years!)

Lecture 1 General relativity and cosmology. Kerson Huang MIT & IAS, NTU

arxiv: v1 [gr-qc] 17 May 2008

Electromagnetic Field and Gravity Waves

Nonsingular big-bounce cosmology from spin and torsion

The One-World-Per-Observer Paradigm of Modern Cosmology

The Concept of Inflation

Physics 314 (Survey of Astronomy) Exam 3

Ghost Bounce 鬼跳. Chunshan Lin. A matter bounce by means of ghost condensation R. Brandenberger, L. Levasseur and C. Lin arxiv:1007.

2.5.1 Static tides Tidal dissipation Dynamical tides Bibliographical notes Exercises 118

The Search for the Complete History of the Cosmos. Neil Turok

Fundamentals of Atmospheric Modelling

Cosmology. Chapter 18. Cosmology. Observations of the Universe. Observations of the Universe. Motion of Galaxies. Cosmology

Lecture XIX: Particle motion exterior to a spherical star

Structure formation. Yvonne Y. Y. Wong Max-Planck-Institut für Physik, München

Holography Duality (8.821/8.871) Fall 2014 Assignment 2

Physics 133: Extragalactic Astronomy ad Cosmology

RELG - General Relativity

Limitations of Newtonian Physics

Fundamental Theories of Physics in Flat and Curved Space-Time

Lecture #25: Plan. Cosmology. The early Universe (cont d) The fate of our Universe The Great Unanswered Questions

A Theory of Gravitation in Flat Space-Time. Walter Petry

Big Bounce and Inflation from Spin and Torsion Nikodem Popławski

Dark Energy vs. Dark Matter: Towards a unifying scalar field?

Propagation of Gravitational Waves in a FRW Universe. What a Cosmological Gravitational Wave may look like

Theory of General Relativity

Hawking s genius. L. Sriramkumar. Department of Physics, Indian Institute of Technology Madras, Chennai

Outline. The Cosmological Principle II. The Perfect Cosmological Principle. The cosmological principle. Covers chapter 2 + half of chapter 3 in Ryden

B.Sc. (Semester - 5) Subject: Physics Course: US05CPHY01 Classical Mechanics

Black Hole Cosmology in Gravity with Torsion Nikodem Popławski

IoP. An Introduction to the Science of Cosmology. Derek Raine. Ted Thomas. Series in Astronomy and Astrophysics

Are naked singularities forbidden by the second law of thermodynamics?

Electromagnetic Field Energy

Answers to Problem Set Number 04 for MIT (Spring 2008)

Moment of beginning of space-time about 13.7 billion years ago. The time at which all the material and energy in the expanding Universe was coincident

ESCI 485 Air/Sea Interaction Lesson 1 Stresses and Fluxes Dr. DeCaria

Non-singular quantum cosmology and scale invariant perturbations

Final Review Prof. WAN, Xin

Fundamentals of Fluid Dynamics: Elementary Viscous Flow

Computational Physics and Astrophysics

Physics of Subspace Geometry

II Relationship of Classical Theory to Quantum Theory A Quantum mean occupation number

Rapid Inflation of the Early Universe. 27. Exploring the Early Universe. The Isotropy Problem. Possible Causes of Cosmic Inflation

On Fluid Maxwell Equations

3. It is expanding: the galaxies are moving apart, accelerating slightly The mystery of Dark Energy

Turbomachinery & Turbulence. Lecture 2: One dimensional thermodynamics.

What is Reality in a Holographic World?

Black Holes and Wave Mechanics

Advanced Newtonian gravity

Gravitation. Adrian Ferent. This is a new quantum gravity theory which breaks the wall of Planck scale. Abstract

5.5 Energy-momentum tensor

Contents. Part I The Big Bang and the Observable Universe

Agenda. Chapter 17. Cosmology. Cosmology. Observations of the Universe. Observations of the Universe

Getting started: CFD notation

PRINCIPLES OF PHYSICS. \Hp. Ni Jun TSINGHUA. Physics. From Quantum Field Theory. to Classical Mechanics. World Scientific. Vol.2. Report and Review in

Section 2: Lecture 1 Integral Form of the Conservation Equations for Compressible Flow

Cosmology. Big Bang and Inflation

n v molecules will pass per unit time through the area from left to

Advanced Study, 9 Adela Court, Mulgrave, Victoria 3170, Australia

Transcription:

Newtonian Gravitation of Matter and Antimatter Claes Johnson January, 0 Abstract We present a cosmological model based on Euler s equation for a self-gravitating medium consisting of matter and antimatter of density ρ generated by a gravitational potential φ as ρ = φ, with presence of matter where φ > 0 with visible matter at singularities and dark matter in regions of smoothness, and antimatter where φ < 0. Lack of Unified Field Theory Modern physics is troubled by the perceived incompatibility of the general theory of relativity for gravitation with Maxwell s equations for electromagnetics and quantum mechanics, which results from the fact that general relativity is a geometric theory of curved space-time while electro/quantum mechanics cannot be given such a geometric form. In particular, there is no unified field theory including both gravitation, fluid dynamics and electromagnetics, which can serve as a cosmological model. Since Newtonian gravitation is compatible with electro/quantum mechanics, it is natural to ask if there is some form of Newtonian gravitation which can replace general relativity in a unified field theory. In this note we explore what a Newtonian fluid model can offer towards a unified field theory in the form of self-gravitating magnetohydrodynamics. The Euler Equations with Gravitation We consider a cosmological model in Euclidean space-time coordinates (x, t) of matter and antimatter subject to gravitation defined by a gravitational potential φ connected to matter/antimatter density ρ by the equation ρ = φ, where is the Laplace operator and matter is present where φ > 0, antimatter present where φ < 0 and there is vacuum where φ = 0. We thus consider a Newtonian model in flat space-time with a generalized gravitational potential φ with φ both positive and negative. We adopt the Euler equations for a compressible perfect gas subject to gravitation expressing conservation of matter/antimatter density ρ, momentum m = ρu and inter-

nal energy e: Find (φ, m, e) as functions of (x, t) such that for t > 0 and all x ρ + m = 0, ṁ + (mu) + p + ρ φ = 0, ė + (eu) + p u = 0, ρ = φ, φ(x, 0) = φ 0 (x), m(x, 0) = m 0 (x), e(x, 0) = e 0 (x), where u = m ρ is matter/antimatter velocity, p = γe is pressure with γ 0 a gas constant, v = v t and (φ0, m 0, e 0 ) given initial values. With φ > 0 this is the usual Euler equations for a prefect self-gravitating gas assuming φ 0 > 0 corresponding to the presence of only matter initially. The novelty here is that φ 0 is allowed to be also negative corresponding to the presence of both matter an antimatter initially. We emphasize that we view the gravitational potential φ as a primary dependent variable with the density ρ = φ as a derived quantity with matter present where φ > 0 and antimatter present where φ < 0. We may view the initial value φ 0 as a perturbation of zero generating both matter and antimatter as out of nothing, like writing 0 = + -. We now turn to a basic conceptual analysis of the model, assuming first that γ = 0 so that p = 0. 3 Concentration-Thinning The momentum equation can alternatively be expressed as Newton s nd law in the form ρ Du = ρ φ, () where Dv v + u v is the material time derivative. Matter/antimatter is thus subject to a gravitational force ρ φ in the direction of decreasing φ thus towards local minima of φ typically associated with φ > 0 and thus presence of matter, and away from local maxima associated with φ < 0 and presence of antimatter. The gravitational force is thus directed inward for matter regions and outward for antimatter regions. The effect of the gravitational force is thus a tendency of concentration of matter with u < 0 and thinning of antimatter with u > 0. This connects to conservation of matter/antimatter expressed as Dρ = ρ u (3) where we see ρ increasing where u < 0 and ρ decreasing where u > 0. 4 Visible and Dark Matter We identify visible matter with point singularities at a point ˆx of the gravitational potential φ of the basic form φ(x) x ˆx corresponding to matter density as a ()

delta-function at ˆx. We refer to smooth φ > 0 as dark matter and thus decompose matter into visible matter and dark matter. The formation of visible matter connects to concentration of matter regions in gravitational collapse. 5 Repulsion Matter-Antimatter We have seen that a matter region tends to concentrate and thus two matter regions not separated by antimatter will attract each other. On the other hand, the attractive force between two matter regions is diminshed if there is an antimatter region in between because of its outward gravitational force. This effect can be interpreted as an effect of repulsion between matter and antimatter which comes out as repulsion between matter regions separated by antimatter. This connects to the observed apparent repulsion between galaxies separated by large voids causing an apparent expansion of the Universe by dark energy [3, 4], if the large voids are identified as regions of antimatter. 6 Action at Distance vs Local Differentiation We here view the gravitational potential φ as the primary variable, from which matter/antimatter density ρ is generated by differentiation as ρ = φ, and not as usual matter density as given from which the gravitational potential is generated by solving or integrating the differential equation φ = ρ with ρ 0. In the first case the generation is a local operation of differentiation while in the second case it is global with action at distance. Viewing the gravitational potential as given thus relieves us from the seemingly impossible task of explaining action at distance. 7 nd Law Solutions of () satisfy a nd law of thermodynamics of the form ([, ]): K = W D + P, Ė = W + D, D 0, (4) where, assuming first the presence of only matter with φ 0, K = ρ u dx, E = e dx, W = p u dx = p u dx, P = ρ φ u dx = φ m dx = φ ρ dx = Φ, Φ = φ φ dx = φ dx, 3

and D is turbulent dissipation. By summation d (K + E Φ) = 0 dt stating that the total energy, the sum of kinetic energy K, heat energy E and gravitational energy Φ, is conserved. This formulation of the nd is fundamentally the same as a formulations in terms of entropy, with the advantage that turbulent dissipation has a clear physical significance while entropy remains mysterious, as explained in detail in []. In gravitational collapse the intensity φ of the gravitational energy Φ increases locally, with corresponding increase of kinetic energy K and transfer to internal heat energy E causing pressure increase until balance with the gravitational force. With also antimatter present with φ < 0, we have (modulo boundary terms) Φ = φ dx φ dx, + where + indicates integration over the domain with φ 0, and over φ < 0. We notice the the gravitational energy of antimatter is positive securing a smooth distribution in accordance with thinning. 8 Generalization to Finite Speed of Propagation It is natural to consider a generalization of Poisson s equation ρ = φ into a wave equation ρ = φ φ (5) c where c represents a finite speed of propagation of gravitation, with corresponding Euler equations ρ + m = 0, ṁ + (mu) + p + ρ φ = 0, (6) ė + (eu) + p u = 0, c φ φ = ρ, together with initial values for ρ, m, e, φ and φ. In this case all variables (ρ, φ, m, e) appear with time-derivate and can be updated computationally by time-stepping. We can view (6) as a relaxation of () corresponding to using a retarded potential. With proper choice of the speed of propagation c, this model can be made to conform with the observed anomalous precession of the perihelion of Mercury, which thus does not require general relativty. Relaxation with instead a parabolic equation of the form is also thinkable. φ φ = ρ, (7) c 4

9 Summary. Matter/antimatter of (non-negative) density ρ is generated from a gravitational potential φ as ρ = φ with presence of matter where φ > 0 and antimatter where φ < 0 and vacuum where φ = 0.. In matter regions visible matter may be associated with singularies of φ and dark matter with regions of smoothness of φ. 3. The gravitational force given by φ is directed inward for matter regions causing concentration and outward for antimatter regions causing thinnning with an effect of repulsion between matter and antimatter thus representing dark energy. 4. The initial value φ 0 with φ of both signs may be viewed as a perturbation from zero with equal amounts of matter and antimatter. 5. With relaxation to finite speed of propagation of gravitation, the model conforms with the observed precession of Mercury. 6. The model appears to include both dark matter and dark energy as effects of a gravitational potential φ with φ of both signs, and allows a start from a perurbation of zero rather than from a Big Bang. References [] J.Hoffman and C. Johnson, Computational Turbulent Incompressible Flow, Springer, 008. [] J.Hoffman, C. Johnson and Murtazo Nazarov, Computational Thermodynamics, to appear. [3] L. Amendola and S. Tsujikawa, Dark Energy, Theory and Observations, Cambridge University Press, 00. [4] Yun Wang, Dark Energy, Wiley 00. 5