A Critique of time dilation Roger J Anderton

Similar documents
Light and Projectiles

Absolute motion versus relative motion in Special Relativity is not dealt with properly

Einstein did not derive E=mc 2 from Special Relativity

College Physics B - PHY2054C. Special Relativity 11/10/2014. My Office Hours: Tuesday 10:00 AM - Noon 206 Keen Building.

Topics: Relativity: What s It All About? Galilean Relativity Einstein s s Principle of Relativity Events and Measurements

Space, Time and Simultaneity

College Physics B - PHY2054C. Special & General Relativity 11/12/2014. My Office Hours: Tuesday 10:00 AM - Noon 206 Keen Building.

Einstein s simple derivation of Lorentz transformation: a critique Roger J. Anderton

The Myth of Dirac supposedly combining Special Relativity with Quantum Mechanics Roger J. Anderton

SPH4U UNIVERSITY PHYSICS

Special Theory of Relativity. A Brief introduction

Special Theory of Relativity. The Newtonian Electron. Newton vs. Einstein. So if Newtonian Physics is wrong. It is all Relative.

CHAPTER 2 Special Theory of Relativity-part 1

Algebra Exam. Solutions and Grading Guide

Scientific Examination of Relativistic Velocity and Acceleration Addition. Copyright 2010 Joseph A. Rybczyk

Chapter 37. Relativity. PowerPoint Lectures for University Physics, 14th Edition Hugh D. Young and Roger A. Freedman Lectures by Jason Harlow

Special Theory of Relativity Prof. Dr. Shiva Prasad Department of Physics Indian Institute of Technology, Bombay

Relativity. Transcript.

ENTER RELATIVITY THE HELIOCENTRISM VS GEOCENTRISM DEBATE ARISES FROM MATTER OF CHOOSING THE BEST REFERENCE POINT. GALILEAN TRANSFORMATION 8/19/2016

Einstein for Everyone Lecture 3: Special Relativity

The True Nature of the Special Relativity Light Clock. Copyright 2012 Joseph A. Rybczyk

Welcome back to PHY 3305

Bell s spaceship paradox

Correct Resolution of the Twin Paradox

RELATIVITY. The End of Physics? A. Special Relativity. 3. Einstein. 2. Michelson-Morley Experiment 5

Superposition - World of Color and Hardness

Lecture 7: Special Relativity I

Lecture 10: General Relativity I

The Greatest Failure of the Scientific Method - Special Relativity. Copyright Joseph A. Rybczyk

dt = p m, (2.1.1) dt = p

2.1 The Ether and the Michelson-Morley Experiment

Lecture 2 - Length Contraction

Special Theory Of Relativity Prof. Shiva Prasad Department of Physics Indian Institute of Technology, Bombay

Simultaneity And Time Dilation

4/13/2015. Outlines CHAPTER 12 ELECTRODYNAMICS & RELATIVITY. 1. The special theory of relativity. 2. Relativistic Mechanics

Einstein takes a bashing because of Higgs Ether Roger J Anderton

Lecture 8 : Special Theory of Relativity

The Constancy of the Speed of Light

JF Theoretical Physics PY1T10 Special Relativity

Baxter s Railroad Company.

Special Relativity 05/09/2008. Lecture 14 1

Recap: Eddington s observation was the first (of very few) piece(s) of (new) evidence for GR

Kinematics of special relativity

E = mc 2. Inertial Reference Frames. Inertial Reference Frames. The Special Theory of Relativity. Slide 1 / 63. Slide 2 / 63.

Velocity Composition for Dummies. Copyright 2009 Joseph A. Rybczyk

Einstein s theory of special relativity

Black Holes -Chapter 21

Elements of Physics II

The Philosophy of Physics. Special Relativity and Minkowski Spacetime

Chapter 26. Relativity

Relativity. An explanation of Brownian motion in terms of atoms. An explanation of the photoelectric effect ==> Quantum Theory

Modern Physics. Third Edition RAYMOND A. SERWAY CLEMENT J. MOSES CURT A. MOYER

Special Relativity 1

Cosmology - How the Universe Came to Be. PLATO: Cosmology

Physics 225 Relativity and Math Applications. Fall Unit 7 The 4-vectors of Dynamics

0 : Einstein s postulates of Special Relativity

Chapter S3 Spacetime and Gravity. Agenda. Distinguishing Crackpots

Albert Einstein ( )

A most elegant philosophy about the Theory Of Everything

Special Theory of Relativity. PH101 Lec-3

Introduction to Relativity & Time Dilation

Relativity. Overview & Postulates Events Relativity of Simultaneity. Relativity of Time. Relativity of Length Relativistic momentum and energy

Did you read chapter 7? Housekeeping. Special Relativity Postulates. Famous quotes from Einstein. Symmetry. (Special Principle of Relativity) 5/9/2007

Your (primed) frame frame

Strange Misconceptions of Gerald t Hooft Roger J Anderton

Redefining Einstein s Velocity Addition Formula. Copyright 2010 Joseph A. Rybczyk

Notes - Special Relativity

Michael Fowler, UVa Physics, 12/1/07. Momentum has Direction

Relativity. Astronomy 101

Postulates of Special Relativity

Lecture 13 Notes: 07 / 20. Invariance of the speed of light

Chapter Two. A Logical Absurdity? Common sense is that layer of prejudices laid down in the mind prior to the age of eighteen -A.

Lecture 12 Notes, Electromagnetic Theory II Dr. Christopher S. Baird, faculty.uml.edu/cbaird University of Massachusetts Lowell

Midterm Solutions. 1 1 = 0.999c (0.2)

The Lorentz Transformation from Light-Speed Invariance Alone

Avoiding the Block Universe: A Reply to Petkov Peter Bokulich Boston University Draft: 3 Feb. 2006

Elements of Physics II

Einstein for Everyone Lecture 4: Paradoxes; Minkowski Spacetime

Chapter 3 Time dilation from the classical wave equation. from my book: Understanding Relativistic Quantum Field Theory.

RELATIVITY. Einstein published two theories of relativity. In The Special Theory. For uniform motion a = 0. In The General Theory

One sided tests. An example of a two sided alternative is what we ve been using for our two sample tests:

Mr Green sees the shorter, straight, green path and Mr. Red sees the longer, curved, red path.

The result is; distances are contracted in the direction of motion.

Light and Relativity

Astronomy 120 Overview

Special relativity, 3. How big is gamma? The Lorentz transformations depend on the factor γ =

Conversation with Tom Bailey about how a photon can have momentum even though it has zero mass 9 September 2012 at 17:57

Gravity and Spacetime: Why do things fall?

The Lorentz Transformation

( ) 2 + v t B = 2 D2 + L 2. = 2D c. t B. & t A. , L = v t B. D = c t A. + v t. = t A. = 2 c. c 2. ( v2 c ) = t. 1 v2. t B 2 = t A.

Einstein s Time Dilation Experiment By Harry H. Ricker III

Pendulum Activity! Frequency, Length, and Gravity. Materials

Physics 280 Lecture 2

The Lorentz Transformations

The interpretation is that gravity bends spacetime and that light follows the curvature of space.

Review Special Relativity. February 3, Absolutes of Relativity. Key Ideas of Special Relativity. Path of Ball in a Moving Train

Physics 280 Closing Arguments

Extra notes on rela,vity. Wade Naylor

Theory of Everything by Illusion 2.0

We saw last time how the development of accurate clocks in the 18 th and 19 th centuries transformed human cultures over the world.

Transcription:

A Critique of time dilation Roger J Anderton R.J.Anderton@btinternet.com Supposedly time dilation can be derived from the postulate of lightspeed constancy alone without the principle of relativity. However this derivation suffers from the same sort of mathematical mistakes in Special relativity. I will go through one such derivation highlighting the mistakes. My source of information for this derivation is wikipedia article on time dilation (Dec 2008). Wikipedia articles keep changing so I provide as reference at the end the article for comparison to this article. The mistakes in that wikipedia article appear to me to be similar to the type of mistakes made in all special relativity articles at this moment in time. We start the derivation from granting the postulate of the constancy of lightspeed and then proceed to the maths. The diagrams used are: Observer at rest sees time 2L/c

Observer moving parallel relative to setup, sees longer path, time > 2L/c, same speed c The article starts: Wikipedia: Time dilation can be inferred from the constancy of the speed of light in all reference frames as follows: Consider a simple clock consisting of two mirrors A and B, between which a light pulse is bouncing. The separation of the mirrors is L, and the clock ticks once each time it hits a given mirror. In the frame where the clock is at rest (diagram at right), the light pulse traces out a path of length 2L and the period of the clock is 2L divided by the speed of light: From the frame of reference of a moving observer traveling at the speed v (diagram at lower right), the light pulse traces out a longer, angled path. The second postulate of special relativity states that the speed of light is constant in all frames, which implies a lengthening of the period of this clock from the moving observer's perspective. That is to say, in a frame moving relative to the clock, the clock appears to be running slower. Straightforward application of the Pythagorean theorem leads to the well-known prediction of special relativity: The total time for the light pulse to trace its path is given by My comment: Really everything in the O frame should have a dash put to it. So it should be c but is assuming c = c. In O frame should be D but in O frame D =0, so going with what the article gives for the moment.

Wikipedia: The length of the half path can be calculated as a function of known quantities as My comment: This is assuming that L = L. Everything observed by O should have dash with it. Anyway, Wikipedia article claims L observed by O equals L observed by L, so uses just L. Wikipedia : Substituting D from this equation into the previous, and solving for t' gives: and thus, with the definition of t: which expresses the fact that for the moving observer the period of the clock is longer than in the frame of the clock itself. My comment: However for the distance L from O it is still covered in time ½ delta t. So have D covered in time ½ delta t and L covered in time ½ delta t in the given diagram.. Point on the mirror B is reached supposedly in two different times ½ delta t and ½ delta t. But that s in the same frame of O so it must happen at the same time interval; which means time interval of delta t = delta t. But then if that s true, it means that the assumption c = c is wrong.

It is not delta t = 2D/c as given by wikipedia; it is instead delta t = 2D/c And c does not equal c. Both O and O measure same value for light speed as c, but c is not c. It s a fundamental error in the dealing with lightspeed. We have expanding circle in frame of O along D the crests of the light wave are moving at speed c, but along L they are not!

O and O are agreeing that the time taken to cover distance L is ½ delta t. But O thinks he is measuring c, when O says you are not, you are measuring c. O is claiming to measure c along L. Both O and O measure what they think is the same value for lightspeed, but they are disagreeing about the other measuring it. There is thus no time dilation. This subtle point gets entirely missed by those muddling the maths. i.e by a total inability of handling the maths of Pythagorean theorem. Complementary fudging enables the deficit of obtaining this false time dilation effect to be cancelled out when it comes to some experiments; while for other experiments the effect is believed and believed measured without the complementary fudging to cancel it. i.e mistakes are not corrected, instead more mistakes are added that sometime cancel out the existing mistakes. The postulate of the constancy of lightspeed (under the relevant conditions of being in vacuum free of gravity and other influences) leads to no time dilation, instead there is disagreement between observers as to how lightspeed is to be measured. However, the massive publicity campaign for the genius of Einstein ensures that this deficit of time dilation stays firmly embedded within physics. Conclusion The trouble with what happens is -- the physicists just mess up the maths, instead of correcting maths mistakes, they just pile them one on top of the other. They even award Nobel prizes for messing up the maths -- cancel out infinities and replace them by finite numbers -- mathematical nonsense -- but call it renormalisation and you get a Nobel Prize in physics. i.e. they are getting rewarded for being rubbish at maths. I think I might have pieced together what happens. At the moment it is only supposition and I have not fully checked it out. But I think the scenario is possibly like this-- The two postulates --relativity principle + "light speed as constant" (under relevant conditions and extras) gives both the maths of Galilean relativity and Special relativity. But what hides that fact is that the maths for Special relativity is derived wrong. i.e. Special relativity is a vast body of mathematical mistakes.

If you were to do the maths correctly then it would be the same maths as Galilean relativity. i.e. the same postulates give the Galilean transform (of Galilean relativity) and do the maths incorrectly from those postulates and you get the Lorentz transform (of Special relativity). I find that idea mind-boggling. Galilean relativity and Special relativity are probably the same theory in the sense that they can be formed from the same postulates, but do the maths correctly from the postulates and you get one theory, do it wrong and you get the other theory. If we grant this supposition as correct, then there is an extra feature. In the way that Galilean relativity has been formed, the idea is that all observers measure the same time intervals. While in Special relativity the idea is that all observers measure the same light speed. (This is of course under the relevant conditions of light speed in vacuum, free of influence by gravity etc.) So, I suspect the maths is the same for both theories except one interprets that maths from universal time and the other from universal light speed. I have not fully checked this idea; mainly because the relativity literature is so vast it is difficult to check through it all. It raises a perplexing problem if a theory consists mainly of mathematical mistakes (such as I now suspect Special relativity) if one starts correcting all of those mistakes so that the theory looks completely different with its maths then it originally did; when does it stop being that theory??? i.e. correct all the mistakes in a theory and it then turns into the same maths as another theory is it still then its original theory? Anyway, what I have established so far in this article as regards time dilation- What happens is that they (the mainstream relativists) do the maths wrong and then create time dilation which isn't really there, then do more maths mistakes to compensate for that maths mistake, and hay presto you have a lot of maths that looks different to Newtonian physics, but most of the wrong stuff cancels out when you test it by experiment. So, they then start proclaiming how clever they are with a theory and its maths that matches observations and data. But it does not fully fit all observations and data so they have to do the maths wrong again to create a supposedly new theory which matches some experiments and observations, but not all, so they have to bodge the maths yet again... and again... and again - creating new theories based on maths bodges and each step of the way congratulating themselves and awarding themselves a Nobel prize for how clever they are. i.e. they have learnt that money is made in doing the maths wrong. Mainstream physics is a vast pile of mathematical mistakes upon which more mathematical mistakes are added; just like adding epicycles to the Ptolemaic model

before the Copernican revolution i.e. their method is - don t correct the existing mathematical problem just add another mathematical bodge to try to make it fit better with experiment. And when anyone tries to make sense of it, well it s a nightmare, and you are liable to get diverted onto numerous dead-ends created by these mistakes. c. RJAnderton2008 Reference from wikipedia Simple inference of time dilation Time dilation can be inferred from the constancy of the speed of light in all reference frames as follows: Consider a simple clock consisting of two mirrors A and B, between which a light pulse is bouncing. The separation of the mirrors is L, and the clock ticks once each time it hits a given mirror. In the frame where the clock is at rest (diagram at right), the light pulse traces out a path of length 2L and the period of the clock is 2L divided by the speed of light: From the frame of reference of a moving observer traveling at the speed v (diagram at lower right), the light pulse traces out a longer, angled path. The second postulate of special relativity states that the speed of light is constant in all frames, which implies a lengthening of the period of this clock from the moving observer's perspective. That is to say, in a frame moving relative to the clock, the clock appears to be running slower. Straightforward application of the Pythagorean theorem leads to the well-known prediction of special relativity: The total time for the light pulse to trace its path is given by The length of the half path can be calculated as a function of known quantities as

Substituting D from this equation into the previous, and solving for t' gives: and thus, with the definition of t: which expresses the fact that for the moving observer the period of the clock is longer than in the frame of the clock itself. Observer at rest sees time 2L/c Observer moving parallel relative to setup, sees longer path, time > 2L/c, same speed c