Sagnac(1913) completed by Dufour & Prunier(1942)

Similar documents
PHY1020 BASIC CONCEPTS IN PHYSICS I

Using light scattering method to find The surface tension of water

Physical Principle of Formation and Essence of Radio Waves

Interference. Physics 102 Workshop #3. General Instructions

Physics 9e/Cutnell. correlated to the. College Board AP Physics 1 Course Objectives

9/16 Optics 1 /11 GEOMETRIC OPTICS

EXPERIMENT O-6. Michelson Interferometer. Abstract. References. Pre-Lab

Sample Questions for the AP Physics 1 Exam

Diffraction of a Circular Aperture

Einstein s Theory of Special Relativity Made Relatively Simple!

Centripetal Force. This result is independent of the size of r. A full circle has 2π rad, and 360 deg = 2π rad.

Fraunhofer Diffraction

PEDAGOGY: THE BUBBLE ANALOGY AND THE DIFFERENCE BETWEEN GRAVITATIONAL FORCES AND ROCKET THRUST IN SPATIAL FLOW THEORIES OF GRAVITY *

Pre-lab Quiz/PHYS 224 Magnetic Force and Current Balance. Your name Lab section

Experiment 3 Lenses and Images

AP1 Waves. (A) frequency (B) wavelength (C) speed (D) intensity. Answer: (A) and (D) frequency and intensity.

E/M Experiment: Electrons in a Magnetic Field.

Chapter 5 Using Newton s Laws: Friction, Circular Motion, Drag Forces. Copyright 2009 Pearson Education, Inc.

Geometric Optics Converging Lenses and Mirrors Physics Lab IV

The purposes of this experiment are to test Faraday's Law qualitatively and to test Lenz's Law.

circular motion & gravitation physics 111N

Theory of electrons and positrons

Rotation: Moment of Inertia and Torque

AP1 Oscillations. 1. Which of the following statements about a spring-block oscillator in simple harmonic motion about its equilibrium point is false?

Holography 1 HOLOGRAPHY

COMPETENCY GOAL 1: The learner will develop abilities necessary to do and understand scientific inquiry.

Online Courses for High School Students

Energy, Work, and Power

Torque and Rotary Motion

Rotational Inertia Demonstrator

AP2 Magnetism. (c) Explain why the magnetic field does no work on the particle as it moves in its circular path.

Physics 41, Winter 1998 Lab 1 - The Current Balance. Theory

What Do You Think? For You To Do GOALS

Lab #4 - Linear Impulse and Momentum

Rutgers Analytical Physics 750:228, Spring 2016 ( RUPHY228S16 )

Chapter 1 Units, Physical Quantities, and Vectors

Linear Motion vs. Rotational Motion

The Special Theory of Relativity

Table 1 r (m) I (W/m 2 ) Table 2: Intensities at 1-m Distances Power (W)

Gravitation and Newton s Synthesis

FTIR Instrumentation

The Viscosity of Fluids

P R E A M B L E. Facilitated workshop problems for class discussion (1.5 hours)

Fluid Mechanics Prof. S. K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur

8.1 Radio Emission from Solar System objects

PHYSICS FOUNDATIONS SOCIETY THE DYNAMIC UNIVERSE TOWARD A UNIFIED PICTURE OF PHYSICAL REALITY TUOMO SUNTOLA

Mechanical Principles

ATOMIC SPECTRA. Apparatus: Optical spectrometer, spectral tubes, power supply, incandescent lamp, bottles of dyed water, elevating jack or block.

Information regarding the Lockheed F-104 Starfighter F-104 LN-3. An article published in the Zipper Magazine #48. December Theo N.M.M.

FORCE ON A CURRENT IN A MAGNETIC FIELD

Force on Moving Charges in a Magnetic Field

Special Relativity. Photo by Philippe Halsman. Used with permission from Mrs. P. Halsman.

Diffraction and Young s Single Slit Experiment

LAB 6: GRAVITATIONAL AND PASSIVE FORCES

A METHOD OF CALIBRATING HELMHOLTZ COILS FOR THE MEASUREMENT OF PERMANENT MAGNETS

Interferometers. OBJECTIVES To examine the operation of several kinds of interferometers. d sin = n (1)

Chapter 1 Mach s Principle and the Concept of Mass

AP Physics B Ch. 23 and Ch. 24 Geometric Optics and Wave Nature of Light

Force measurement. Forces VECTORIAL ISSUES ACTION ET RÉACTION ISOSTATISM

Measurement of Charge-to-Mass (e/m) Ratio for the Electron

Center of Gravity. We touched on this briefly in chapter 7! x 2

Physics 111: Lecture 4: Chapter 4 - Forces and Newton s Laws of Motion. Physics is about forces and how the world around us reacts to these forces.

Centripetal force, rotary motion, angular velocity, apparent force.

Name Class Date Laboratory Investigation 4B Chapter 4: Cell Structure

Simple Harmonic Motion

ElectroMagnetic Induction. AP Physics B

Optics. Kepler's telescope and Galileo's telescope. f 1. f 2. LD Physics Leaflets P Geometrical optics Optical instruments

Lab 7: Rotational Motion

Physics 25 Exam 3 November 3, 2009

Candidate Number. General Certificate of Education Advanced Level Examination June 2014

Acceleration due to Gravity

Salem Community College Course Syllabus. Course Title: Physics I. Course Code: PHY 101. Lecture Hours: 2 Laboratory Hours: 4 Credits: 4

Chapter 10 Rotational Motion. Copyright 2009 Pearson Education, Inc.

The Three Heat Transfer Modes in Reflow Soldering

Reflection and Refraction

Lecture 16. Newton s Second Law for Rotation. Moment of Inertia. Angular momentum. Cutnell+Johnson: 9.4, 9.6

Experiment 5 ~ Friction

The Neo-classical Theory of Relativity

Tennessee State University

Chapter 7 Newton s Laws of Motion

Physics 221 Classical Physics II Lab Gustavus Adolphus College Spring 2007

The University of Texas at Austin. Gravity and Orbits

Version A Page The diagram shows two bowling balls, A and B, each having a mass of 7.00 kilograms, placed 2.00 meters apart.

A Fishy Tale. Observing the Circulatory System of a Goldfish with a Compound Light Microscope

Newton s Law of Universal Gravitation

Lab 8: Ballistic Pendulum

Experimental Uncertainties (Errors)

Physics 112 Homework 5 (solutions) (2004 Fall) Solutions to Homework Questions 5

Deformation of the Bodies by the Result of Length Contraction: A new Approach to the Lorentz Contraction

All About Motion - Displacement, Velocity and Acceleration

ENGINEERING METROLOGY

Awell-known lecture demonstration1

GLOBAL COLLEGE OF ENGINEERING &TECHNOLOGY: YSR DIST. Unit VII Fiber Optics Engineering Physics

Modern Classical Optics

Convex Mirrors. Ray Diagram for Convex Mirror

Physics 160 Biomechanics. Angular Kinematics

SOLID MECHANICS TUTORIAL MECHANISMS KINEMATICS - VELOCITY AND ACCELERATION DIAGRAMS

Introduction to Fourier Transform Infrared Spectrometry

Transcription:

Sagnac(1913) completed by Dufour & Prunier(1942) Robert Bennett robert.bennett@rcn.com Abstract The 1913 Sagnac test proved to be a critical experiment that refuted Special Relativity (as Sagnac intended) and supported a model of aether that could be entrained like material fluids. But it also generated more questions, such as: What is the Speed of Light(SoL) in the lab frame? What if the optical components of the interferometer were moving relative to each other..some in the lab frame, some in the rotor frame testing the emission model of light transmission? What if the half beams were directed above the plane of the rotor? All these questions were answered in an extension of the Sagnac test done 29 years after the SagnacX by D&P. An analytic review of On a Fringe Movement Registered on a Platform in Uniform Motion (1942). Dufour and F. Prunier J. de Physique. Radium 3, 9 (1942) P 153-162 On a Fringe Movement Registered on a Platform in Uniform Motion (1942). A Review.. we used an optical circuit entirely fixed to the rotating platform, as did Sagnac. Under these same conditions we found that the movement of fringes observed are similar within 6%, whether the light source and photographic receiver be dragged in the rotation of the platform, as in the experiments of Sagnac, or they remain fixed in the laboratory. Sagnac and D&P both found SoL = c +- v in the rotor frame. D&P found SoL = c +- v also, in the lab frame (optical bench at rest, empty platform spinning below it) This alone disproves Special Relativity, as SoL <> c

The second series of experiments described here was aimed to explore the fringe displacement due to rotation, in entirely new conditions where the optical circuit of the two superimposed interfering beams is composed of two parts in series, one of which remains fixed in relation to the laboratory while the other is attached to the rotating platform. Moving fringes, obtained under these new conditions, were the same one that allows for the classical Galilean theory. The frame is determined by the location of the detector(film). So parts of the optical system were in relative motion yet the same result was seen SoL = c +- r = c +- v This alone rejects the Ritz emission model, since the last reflection before the detector would determine SoL. But it doesn t; SoL is always Galilean, as above. I. -- Experiments in which the Optical circuit is entirely supported on a Rotary platform. 1. Preliminary experiments. we first of all have repeated the experience of Sagnac [1] in which all the optical apparatus is moving with the disk in uniform rotation. We used the same mirrors as Sagnac in his experiment, but the platform was twice as large as his.. This material arrangement has remained the same for all experiments that will be discussed here. Figure 1 gives the layout of optical apparatus straddling the entire disc and used in these preliminary tests. It is close to identical to that of Sagnac and does nothing original. In spite of some imperfections, the significance of the results obtained remains whole here from the qualitative point of view. Moreover, even from the quantitative point of view, the greatest variations of the numerical results of even one series of recordings never exceeded 13 per 100 of the median value.

2. Experiments made with a source of light remaining fixed in the laboratory. The first question that we considered was to determine if the movement of the source that creates the light is essential to the production of the phenomenon. We then constructed the apparatus as shown in figure 2. The characteristics of this assembly are to use the light of a fixed source in the laboratory and to send this light on the optical courses fixed to the platform in rotation. the light resulting from the source S will traverse the lens l, the diaphragm t and the microscope objective s, all these bodies being maintained fixed to the laboratory. Another microscope objective r identical to the first, is fixed to the revolving platform The recordings which we carried out thus show a net shift of the fringes completely comparable with that provided by the traditional assembly of Sagnac. That is, SoL = c +- v It is seen that to 5 or 6 per 100 precision, the average shift observed is of the same value here than that obtained above with the ordinary assembly of Sagnac.. these last experiments show that it is possible to practically use the light emitted by a source not belonging to the mobile disc system,. for an induced observer in rotation.

3. Experiments made by using a source and a photographic recorder remaining fixed in the laboratory. One could ask whether the interferential phenomenon remains the same as for the observer fixed in rotation and for an observer maintained fixed in the laboratory frame? To carry out this study, the device represented schematically in figure 2 underwent the following modifications: the mirror p was removed, the objective lenses L` and the eyepiece o' as well as the photographic chamber P were removed from the platform and fixed to a support motionless with the wall of the laboratory. In this arrangement, the source of light and the observer operating the photography of the fringes with the lenses and photographic chamber, are both fixed in the laboratory. the fringes obtained on the photographic plate underwent a light modification because the lens and plate are motionless, while the interferometer is turning. he average of the two values for opposite rotations is 0.091 of the distance between interference fringes, differing only from 3 to 4 /100 of the number obtained previously if the source of light were fixed in the laboratory. SoL = c +- v does remain the same, with 3 or 4% error I I. - Experiments in the which optical circuit includes, in series, a fixed part in the laboratory and, a part pulled by the platform in rotation. 2. Device actually used. Fig 6

The preceding disadvantages resulted owing to the fact that the two interfering beams followed distinct paths. They disappeared when we obliged the two beams to follow the same course in opposite directions. Figure 6 gives, in perspective, the diagram of the apparatus construction which was useful to us.. 8 Mirrors G, H, I remain fixed in the laboratory. the source (not drawn), is fixed in the laboratory. Note that the 2 half-beams reflect to 20 cm above the rotor and then travel 2 radii. 3. Experimental results. These experiments highlight the existence, under these conditions, of a shift of the fringes of approximately 0.056 distance between interference fringes in white light, for the two directions of rotation and an angular speed of 1 turn/second... the phenomenon is beyond doubt and its cause must be sought in the influence of the number of revolutions of the platform on the propagation of light, using the various possible interpretations. That is what we are going to consider now. III. - Interpretation of the experimental results. Classical Galilean theory supposes that for the observer linked (fixed) to the disc, the speed of the light in a point of the revolving disc differs from the speed C of the light in the laboratory, in a quantity equal to + /- v, if v represents in value the absolute projection of the linear velocity of the disk at the point considered on the platform. That is, SoL = c +- v Part of the optical circuit is fixed to the revolving disc, the other part of the optical circuit remains fixed compared to the laboratory. Under these conditions, which are those of our experiments, the shift of the fringes is due obviously to the optical course fixed to the revolving disc. We will calculate the values which return to us according to the two theories, classical and relativity. The relativistic value is approximately ten times smaller. The relativistic theory thus seems to be in complete dissention with the classical theory and also with the result provided by this experiment. Summary of D&P test We have shown (1) that the experiment provides the same result for the Sagnac effect, whether the observer is entrained or not by the disc. The interpretation of this result appeared to us to present difficulties in relativistic theory. D&P

When rotor is at rest in lab frame: SoL = c in both reference frames When rotor moves at v in lab frame: SoL = c +- v in both reference frames Special Relativity is disproven Emission theory is disproven. Aether entrainment(full dragging) is supported Galilean relativity is supported.conditionally! Consider the lab frame results with CW platform rotation and the CW half beam that produces SoL = c + v. If the rotor drags the surrounding aether at its speed v, then Galilean addition predicts SoL = c + v, as measured. This was Sagnac s insight. Sagnac s test interpretation in quotes The interference of light in a rotating interferometer of a special kind proves to depend on the rotation (with respect to an inertial frame). Sagnac announced this result as a proof of the existence of the ether. Although there still were, in 1913, many physicists to welcome such a claim, the increasingly powerful adepts of relativity theory brushed it away. The Sagnac experiment soon became a textbook classic, and experts in relativity theory felt compelled to explain it both in special and in general relativity. Numerous variants of the experiment have been performed from the interwar period to these days. Interest in the Sagnac effect grew enormously when laser technology turned it into an efficient gyroscopic device. The inertial frame for measuring rotation must be the ECEF or lab frame, as the ALFA theory proves. I showed that an interferometer using a closed optical path enclosing a given area and rotating in the plane of the path, detects the movement of the system relative to the ether in space. Relative motion of aether and optical system does not mean that aether is fixed, but that the system could be fixed and the aether in motion (fluid aether/alfa model) The outcome of these measurements shows that in ambient space, light propagates with speed Vo independent of the motion of the apparatus, the light source and the optical system. This property of space describes the luminiferous ether experimentally.

This is the experimental proof of the whirling relative ether wind that the rotating system creates through its motion. Modern description would call this an aether vortex. In Fresnel s hypothesis of the ether, the half beams CW and CCW to rotation propagate in the ether with a speed Vo independent of the motion of the interferometer. The phase of the CCW beam gives, according to the expression C λvo, a lag x in the phase of the CCW beam, and advances by the same amount the phase of the CW beam propagating in the reverse direction. The Sagnac effect shows the light beams are independent of the motion of the system components but NOT of the aether motion. We may describe luminous phenomena without mentioning the ether. But that is not a satisfactory description.... It does not give the satisfaction we feel by eliminating direct action at a distance. Sagnac s interpretation makes physics local, s the aether and platform motion interact; no action at a distance The observed interferential effect proves to be the optical whirling effect caused by the motion of the system with respect to the ether, and it directly manifests the existence of the ether, necessary carrier of the luminous waves of Huygens and Fresnel. In the new experiment, motion with respect to the ether had a measurable effect, and this effect was of first order in the implied velocities. Sagnac believed he had struck a fatal blow on relativity theory by proving the existence of the ether. The luminous ether is proved by the effect of the relative ether wind in a uniformly rotating interferometer. Sagnac never ceased to see his experiment as a proof of a relative ether whirling... your experiment will always remain a fundamental experiment, even one of the most fundamental experiments of physics. Yet it will not suffice to convince the staunch relativists of the existence of the ether. For the relativists are men who purport to imagine waves that propagate in a medium whose existence they deny. Bjerknes in a letter to Sagnac. ALFA interpretation (Absolute Lab Frame and Fluid Aether) Consider first the lab frame results: SoL = v rotor off SoL = c +- v rotor on

Just as a headwind or a tail wind will add to or subtract from a plane s speed, the light beams obey the Galilean law of velocity addition. But why is the change in light speed v the same as the rotor speed v(at the radius of measurement)? This exhibits full aether dragging by the rotor s mass, producing v = rw in aether speed. sometimes called kinematic entrainment, since dynamics ins not involved. The generalization of this phenomenon would require all motion of matter through aether to drag aether at the same speed full or co-moving drag. Now the rotor frame results: SoL = v rotor off SoL = c +- v rotor on The same as the lab frame. But this raises a logical impasse which is: If the aether is being dragged with the rotor, then it is always co-moving with rotor. The aether frame of reference is at rest relative to the rotor frame. So the aether speed should be measured as v= 0 in the rotor frame. Rotor and aether are comoving, yet the light speed changes by v! In the lab frame aether speed was measured in that frame and aether drag correctly predicted the measured light speed. If aether speed is always measured in the lab frame, then light speed would again be SoL = c +- v! Consistent with other tests( Sagnac(1913) and the Wang FOC test(2005) and Newton s Bucket (1687), the explanation of the D&P rrotor frame result is the absoluteness of the lab frame. All predictions of motion in dynamics must use the lab frame as inertial frame, since inertial frame(s) are defined as those in which the laws of dynamics are valid. But there are not multiple inertial frames, since all reference frames at rest relative to the lab frame are equivalent to it, such as the surface, the interior volume and the geostationary satellites. The enigma of the Sagnac/D&P results is solved by making the Earth the universal frame for predicting future motion using Newton s and Maxwell s laws. References Regarding the Proof for the Existence of a Luminiferous Ether Using a Rotating Inteferometer Experiment G Sagnac - The Abraham Zelmanov Journal, 2008 - zelmanov.ptep-online.com Georges Sagnac: A life for optics https://www.sciencedirect.com/science/article/pii/s1631070514001340