1 Mathematical Theory Of Cosmological Redshift in Static Lobachevskian Universe. Mistake of Edwin Hubble. J. Georg von Brzeski Vadim von Brzeski www.helioslabs.com.

Slides:



Advertisements
Similar presentations
What is The Poincaré Conjecture?
Advertisements

Some Conceptual Problems in Cosmology Prof. J. V. Narlikar IUCAA, Pune.
Maxwell’s Equations from Special Relativity James G. O’Brien Physics Club Presentation University Of Connecticut Thursday October 30th, 2008.
Electromagnetic Waves
So far Geometrical Optics – Reflection and refraction from planar and spherical interfaces –Imaging condition in the paraxial approximation –Apertures.
Red-shift and the Expansion of the Universe. Wavelength - the distance over which a wave repeats itself (a) Longer wavelength; (b) shorter wavelength.
EE3321 ELECTROMAGENTIC FIELD THEORY
Dark Energy. Conclusions from Hubble’s Law The universe is expanding Space itself is expanding Galaxies are held together by gravity on “small” distance.
Gauss’ Law Besides adding up the electric fields due to all the individual electric charges, we can use something called Gauss’ Law. Its idea is similar.
Lecture 20 Hubble Time – Scale Factor ASTR 340 Fall 2006 Dennis Papadopoulos.
Corp. Research Princeton, NJ Cut Metrics and Geometry of Grid Graphs Yuri Boykov, Siemens Research, Princeton, NJ joint work with Vladimir Kolmogorov,
Expanding Universes Intro Cosmology Short Course Lecture 2 Paul Stankus, ORNL.
1 EE 542 Antennas and Propagation for Wireless Communications Array Antennas.
Slipher’s Spectra of Nebulae Lowell Telescope – near Flagstaff Arizona – provided spectra of ~50 nebulae – showing 95% of them were moving away from Earth.
Lecture 23 Models with Cosmological Constant ASTR 340 Fall 2006 Dennis Papadopoulos Chapter 11 Problems Due 12/5/06.
Physics 133: Extragalactic Astronomy ad Cosmology Lecture 4; January
Cosmological Models II Connecting Hubble’s law and the cosmological scale factor What determines the kind of Universe in which we live? The Friedman equation.
Lecture 22 Cosmological Models ASTR 340 Fall 2006 Dennis Papadopoulos Chapter 11.
Observables So far we have talked about the Universe’s dynamic evolution with two Observables –a –the scale factor (tracked by redshift) –t – time So a.
Lecture 21 Cosmological Models ASTR 340 Fall 2006 Dennis Papadopoulos.
By Jaedyn Waggoner. Block C. Mr. Horton. Science 9 THE UNIVERSE.
Kinematics Chapters 2 & 3.
Various Techniques for Measuring Astronomical Distances Alex Blanton 1.
New Core Curriculum week 4, class-2 Foundations of Scientific Process The Birth of the Universe.
The Dynamics of Visible Objects in the Universe.
Review of Vector Analysis
What can electromagnetic waves tell us about the movement of planets, stars, and galaxies?
Theory on the Formation of the Universe
Section 1: Light and Quantized Energy
Cosmology: The Study of the Universe as a Whole Physics 360 Geol 360 Astronomy John Swez.
The Theory/Observation connection lecture 1 the standard model Will Percival The University of Portsmouth.
Cosmology The Origin and Future of the Universe Part I Olbers’ Paradox.
EMR, Big Bang, and Stars Unit Review. Use the pink NECAP reference sheet to answer following questions: 1.What is the relationship between the frequency.
Outline Magnetic dipole moment Magnetization Magnetic induction
EXPANDING UNIVERSE. OLBERS PARADOX Olbers’ paradox “The night sky is dark.” This statement is called Olbers’ paradox, after astronomer who discussed.
Electromagnetic Waves
Dark Energy Wednesday, October 29 Midterm on Friday, October 31.
In the absence of sources, the Maxwell equations in an infinite medium are.
Stars: Binary Systems. Binary star systems allow the determination of stellar masses. The orbital velocity of stars in a binary system reflect the stellar.
THE EXPANSION OF THE UNIVERSE!. Einstein  The discovery of the expansion of the universe was first found by Einstein  -Disagreed with this point- as.
General Relativity Physics Honours 2008 A/Prof. Geraint F. Lewis Rm 560, A29 Lecture Notes 10.
Principle of Equivalence: Einstein 1907 Box stationary in gravity field Box falling freely Box accelerates in empty space Box moves through space at constant.
Nature of Light Physics 1.
10/5/2004New Windows on the Universe Jan Kuijpers Part 1: Gravitation & relativityPart 1: Gravitation & relativity J.A. Peacock, Cosmological Physics,
Hubble’s Law Astrophysics Lesson 16.
Physics 1C Lecture 27A. Interference Treating light as a particle (geometrical optics) helped us to understand how images are formed by lenses and mirrors.
Advanced EM - Master in Physics Poynting’s theorem Momentum conservation Just as we arrived to the Poynting theorem – which represents the.
General Relativity Physics Honours 2008 A/Prof. Geraint F. Lewis Rm 560, A29 Lecture Notes 9.
Ch. 22 Cosmology - Part 1 The Beginning. Beginnings ???? - Newton suggested that for the stars not to have coalesced, the universe must be infinite and.
The Universe BY AMANDA MITCHELL SCIENCE 9, MR HORTON DUE FEBRUARY 25TH.
The Meaning of Einstein’s Equation*
Approaching a final comoving co-ordinate Since the Hubble Flow is defined by the motion of galaxies at fixed comoving co-ordinates a reasonable definition.
PHYS 408 Applied Optics (Lecture 4) JAN-APRIL 2016 EDITION JEFF YOUNG AMPEL RM 113.
Wednesday, Feb. 8, 2012PHYS , Spring 2012 Dr. Jaehoon Yu 1 PHYS 1444 – Section 004 Lecture #7 Wednesday, Feb. 8, 2012 Dr. Alden Stradeling Chapter.
ASTR 113 – 003 Spring 2006 Lecture 12 April 19, 2006 Review (Ch4-5): the Foundation Galaxy (Ch 25-27) Cosmology (Ch28-29) Introduction To Modern Astronomy.
Lecture 14: The Expanding Universe Astronomy 1143 – Spring 2014.
The Fate of the Universe. The fate depends on the rate of expansion and the density Density greater than critical value – gravity will halt expansion.
Option D. 3. Universe was born around 13.8 billion years ago in process called Big Bang In the beginning, all matter & energy in the entire universe was.
Cosmology Scale factor Cosmology à la Newton Cosmology à la Einstein
 You will know the Doppler effect as the falling note of a car or train horn as it approaches, passes, and then goes away from you.
The Cosmological Redshift DEBATE TIME!!!. The spectral features of virtually all galaxies are redshifted  They’re all moving away from us.
Image of the day Turn in cosmology questions!.
Add to table of Contents:
HYPERBOLIC GEOMETRY Paul Klotzle Gabe Richmond.
Astrophysics and Cosmology
Curved spacetime and implications for cosmology
Expansion of the Universe
Expanding Space.
Cosmology.
GTR Continued.
Presentation transcript:

1 Mathematical Theory Of Cosmological Redshift in Static Lobachevskian Universe. Mistake of Edwin Hubble. J. Georg von Brzeski Vadim von Brzeski CCC2 Port Angeles, Washington, USA, September 2008

2 Goals Present a mathematical model of cosmological redshift in static space –Based on our previously published papers [2,3,4,5] Explain cosmological redshift as a physical realization of abstract Lobachevskian geometry [1,6,8] Present an alternative, logically and mathematically coherent, explanation to the “expansion” driven by the Big Bang Analyze Edwin Hubble’s mistake and its legacy

3 Scientifically Required Properties of a Formula for Cosmological Redshift Explain existing observations & extend to new areas Expressed by conceptually coherent, clear & acceptable mathematical formula It should uniformly shift entire spectrum & preserve wavelength ratios It should also be –Scale invariant –Source independent –Linear fn of distance for “small” distances (already experimentally observed)

4 Key Concepts Geodesics –Paths of shortest distances –In physics, commonly identified with rays of light Horospheres in Lobachevskian space. –Spheres of infinite radius (limit spheres) orthogonal to equivalence classes of geodesics having common point at infinity and tangent at that point to the boundary at infinity –Can be interpreted as surfaces of constant phase of EM wave (wavefronts) Mapping of hyperbolic distances onto Euclidean distances

5 Behavior of Parallel Geodesics in Lobachevskian Space Horospheres: Surfaces of constant phase (horespherical wavefronts); orthogonal to geodesics Geodesics – Diverge Exponentially. Volume ~ exp(R) Foliation of L 3 by horospherical waves Ω. Illusion of space “expansion” in astronomy based on E 3. l0l0 l

6 Parallel Geodesics in Euclidean Space Horospheres: Surfaces of constant phase (plane waves) orthogonal to geodesics Parallel Geodesics – Equally spaced l on entire Euclidean space. Volume ~ R n l l l l d d Foliation of E 3 by plane waves Ω.

7 Key Theorem (Lobachevsky): Rate of divergence of geodesics in LG l l0l0 exp(δ) = l0l0 l Theorem gives a novel approach to measuring distance in space without involving the notion of time. Clocks: NO, diffraction gratings: YES. Reference horosphere Parallel geodesics Parallel horospheres Unit radius, R = 1. Poincare ball model of LG.

8 Mapping of Distances in Lobachevskian Space into Euclidean Space d = tanh(δ) –d : Euclidean distance in E 3 –δ : Hyperbolic distance in L 3 Similar to S 2  E 2 Mercator projection via tan() function

9 Formula for Cosmological Redshift Distance Measured by Diffraction Gratings From distance mapping and Lobachevsky’s theorem ln l l0l0 δ = d = tanh(δ) We get the Formula for Cosmological Redshift = tanh(δ) = tanh( ln ( ) ) = tanh( ln (1 + z) ), R = 1. λ λ0λ0 Geodesics separated by λ 0 at source will be separated by λ > λ 0 at detector. and d 1 d R = tanh (ln (1 + z)) Arbitrary R.

10 Properties of Our Model Physical realization of geometrical theorem of abstract LG Uniformly shifts entire spectrum –Preserves wavelength ratios Scale invariant Monotonically increasing fn of distance Linear fn of distance for “small” distances Source independent Easy to compute

11 Relationship of Our Formula to Actual Hubble Observations Our formula : Recalling that for x << 1 ln (1 + x) ~ x tanh(x) ~ x Thus : d R = tanh (ln (1 + z)) d R = z or z = Kd, where K = 1/R This is exactly what Hubble found - redshift is a linear function of distance. Hubble experimentally discovered evidence for Lobachevskian geometry of the Universe and failed to recognize properly what he observed [7].

12 Graphical Representation of tanh(ln(1+z) ln(1+z) tanh( ln(1+z) ) z ≈ KD (Hubble observations) Linear behavior, valid only for small z. (von Brzeski et. al.) Valid for all z, 0 ≤ z < ∞

13 Test of Our Formula for Redshift Our formula: Represent LG by velocity space, i.e. (signed) distance means relative velocity [2,9] Thus, d  v, R  c From the definition of tanh(x), we get: d R = tanh (ln (1 + z)) v c β = = tanh (ln (1 + z)) 1 + β 1 - β 1/2 = λ λ0λ0 1 + z = Relativistic Doppler effect as shown in all references.

14 Hubble’s Mistake and It’s Legacy Hubble measured redshift z and distance d to some objects He found experimentally z = Kd, linear He erroneously assumed z = Cv : the only cause of redshift was the linear Doppler effect Thus, he equated RHS of the above and obtained relationship: v = Hd, called in all literature the Hubble velocity distance “law” But v = Hd has no experimental basis! Slope, H, called the Hubble constant (parameter), is not a physical quantity –Hubble time, Hubble flow as well

15 Application of Our Model NGC 4319 controversy with binary system –Difference in redshift for 2 component spatially localized system z1 = for NGC 4319 z2 = for QSO If we assume NGC 4319 as a reference, and it’s redshift is due only to distance, then Δz = is due to relative velocity v rel = 0.81c –if QSO is located in the galaxy

16 Faint Galaxy Count Data shows that there are more faint galaxies than would follow from Euclidean universe –Euclidean volume ~ R n Natural explanation of faint galaxy count in Lobachevskian universe –Lobachevskian volume ~ exp(R) From the count of faint galaxies in Lobachevskian universe it might be possible to recover distances to them

17 Conclusions Negative curvature of space causes an illusion of the existence of a global velocity field Illusion was interpreted by Hubble and followers as the effect of “space inflation”, which extrapolated backwards led to a singularity mockingly named by F. Hoyle as the Big Bang Observed cosmological redshift, which increases monotonically with distance, is due to Lobachevskian large scale vacuum given by : d R = tanh (ln (1 + z))

18 References 1.Bonola, R., Non-Euclidean Geometry, Dover,NY This book has an original paper by N.I. Lobachevsky 2.von Brzeski, J.G., von Brzeski,V., Topological Frequency Shifts, Electromagnetic Field in Lobachevskian Geometry, PIER 39,p.289, von Brzeski,J.G., von Brzeski,V., Topological Intensity Shifts, Electromagnetic Field in Lobachevskian Geometry, PIER 43, p.161, von Brzeski, J.G., Application of Lobachevsky’s Formula on the Angle of Parallelism to Geometry of Space and to the Cosmological Redshift, Russian Journal of Mathematical Physics, 14,p.366, von Brzeski,J.G., Expansion of the Universe-Mistake of Edwin Hubble? Cosmological Redshift and Related Electromagnetic Phenomena in Static Lobachevskian (Hyperbolic) Universe, Acta Physica Polonica, 39, No.6, p.1501, Buseman,H., Kelly,P.J., Projective Geometry and Projective Metrics, Academic Press, NY, Hubble,E., A Relation Between Distance and Radial Velocity Among Extra Galactic Nebulae, Proc.of National Academy of Sciences, vol.15,No 3, March15, Iversen, B., Hyperbolic Geometry, Cambridge Univ.Press, Smorodinsky, Ya. A., Kinematika i Geomietriya Lobachevskogo, ( Kinematics and Lobachevskian Geometry) in Russian, Atomnaya Energiya 1956, Available from Joint Institute for Nuclear Research Library, Dubna, Russian Ferderation.