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Experimental basis for special relativity

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Title: Experimental basis for special relativity


1
Experimental basis forspecial relativity
  • Experiments related to the ether hypothesis
  • Experiments on the speed of light from moving
    sources
  • Experiments on time-dilation effects
  • Experiments to measure the kinetic energy of
    relativistic electrons

2
The luminiferous ether
  • Mechanical waves, water, sound, strings, etc.
    require a medium
  • The speed of propagation of mechanical waves
    depends on the motion of the medium
  • It was logical to accept that there must be a
    medium for the propagation of light, so that em
    waves are oscillations in the ether
  • Newton, Huygens, Maxwell, Rayleigh all believed
    that the ether existed

3
Consequences of the ether
  • If there was a medium for light wave propagation,
    then the speed of light must be measured relative
    to that medium
  • Thus the ether could provide an absolute
    reference frame for all measurements
  • The ether must have some strange properties
  • it must be solid-like to support high-frequency
    transverse waves
  • yet it had to be of very low density so that it
    did not disturb the motion of planets and other
    astronomical bodies too much

4
The aberration of starlight(James Bradley 1727)
  • Change in the apparent position of a star due to
    changes in the velocity of the earth in its orbit
  • Fresnel attempted to explain this from a theory
    of the velocity of light in a moving medium
  • According to Fresnel, the ether was dragged along
    with the earth and this gave rise to the
    aberration effect
  • However, Einstein gave the correct explanation in
    terms of relativistic velocity addition. A light
    ray will have a different angle in different
    relativistic frames of reference

5
Fizeaus measurements of the speed of light in a
moving fluid (1851)
  • He measured c and got 315,000,000 m/s
  • He used interference effects to attempt to
    measure the speed of light in moving water
  • He expected to measure c v, but the magnitude
    of the result was ltlt expected

6
Michelson-Morley experiment (1887)
  • Attempt to detect the relative motion of matter
    through the ether
  • http//galileo.phys.virginia.edu/classes/109N/lect
    ures/michelson.html
  • Used interference of light due to path length
    differences (fringe shift when apparatus was
    rotated.
  • Found no measurable effect
  • ? NO ETHER

Optical table was a 1½ ton granite slab floating
in a pool of mercury, to minimize the effects of
vibrations, and to allow it to be rotated easily.
7
Einsteins postulates of special relativity
  • I. The laws of physics (mechanics and
    electrodynamics) are valid in all inertial frames
    of reference. There is no absolute frame of
    reference.
  • II. Light is always propagated in empty space
    with a definite velocity c with respect to any
    frame of reference, regardless of the state of
    motion of the emitting body.

8
Faradays law of electromagnetic induction
Einstein was motivated by the fact that the
induced voltage in the coil did not depend on
whether the magnet was moved toward the coil or
if the coil was moved toward the magnet.
9
Test of the second postulate of the special
theory of relativity in the GeV region (Alvager
et al., Phys. Lett. 12, 360, 1984) ? Used the
CERN Proton Synchrotron to accelerate protons to
19.2 GeV/c which then slammed into a Be target
producing ?0 mesons at 6 GeV ? ?? 0.99975. ?
The ?0s decay into 2 photons. A time-of-flight
method was used to measure the photon speed
10
Experimental setup
11
?0 ? ? experiment
  • This amounts to measuring c produced on a source
    (the ?0 s) moving at 0.99975 c
  • Results? c c kv
  • k (?3 ? 13) x 10?5

12
Muon decay and time dilation
  • Muons are produced by decays of ?s in cosmic ray
    collisions with nuclei in the upper atmosphere.
  • The half-life of muons at rest is ?0 1.52 ?s
  • The muons move at 0.98c, so in one ?0 , they
    would travel lt 500 m, and would not be detected
    on earth.
  • Muons are detected on earth

13
Muon decay and time dilation, continued
  • We observe muons on earth because of the
    relativistic time dilation effect.
  • The proper lifetime of the muon is
  • With this lifetime, the muons would travel
    roughly 2.25 km, so some would be detected on
    earth.

14
Measurements of the speed and kinetic energy of
relativistic electrons
  • Classically K ½ m v2, where m constant
  • There is no limit on v, so that if a force
    continually acts on an object, it will eventually
    reach a speed in excess of c, in contradiction to
    Einsteins second postulate.
  • Two types of experiments
  • using relativistic electrons emitted by a
    radioactive source (Am. J. Phys. 77, 757, 2009)
  • Using a Van de Graff device to accelerate
    electrons to high speeds and measuring(Am. J.
    Phys. 32, 551, 1964).

15
Experiment use radioactive source that emits
electrons
S1 and S2 are very thin scintillation detectors
that produce a light Pulse when electrons hit
them. The light pulses measure the time interval
For the electrons to travel the know distance L,
this v is measured. The Kinetic energy of the
electrons emitted by the radioactive nuclei is
known.
16
Experiment using a Van De Graff electron
accelerator
The kinetic energy of the electrons is measured
by the heat produced when they slam into the
aluminum disk at the end (calorimetry). The
calorimeter is calibrated by heating it using a
resistor embedded in the disk. A thermo- couple
is used to measure the increase in temperature.
17
Results Classical physics fails!
Radioactive sources 133Ba (25 - 80 keV) and
207Bi (240 -1047 keV)
18
Results using a linear accelerator
19
Results using the van de Graff
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