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Riding on aLight Beam
Einstein’s SpecialTheory of Relativity
Last time … Discovery of electromagnetism Light as an electromagnetic wave
Frequency, wavelength, amplitude C = f * λ
Spectral lines in light Emission and absorption lines
– Fingerprints of chemical elements Quantum explanation of the lines (Bohr atom)
Light as energy packets (photons) Astrophysics of 1890s
Solar and stellar spectral photography & analysis
Newton and Einstein Both experienced a “Great Year” Both non-typical personalities Both famous during lifetime Both developed new styles of doing
science Both helped define new worldview for
physics and culture more generally
“Classical” reality rejected bythe “moderns” Absolute time and space Measurement unproblematic Deterministic, causal laws Continuously varying processes Objective world, independent of
observer
Albert Einstein (1879-1955) Son of failed businessman Carefree youth in Italy, failed exams Studied physics at ETH Zurich Bern patent officer, 1902-9 Professor in Prague, Zurich, Berlin 1921 Nobel Prize and growing anti-Semitism Emigration to Princeton, 1933 Search for deterministic unified field theory Guru of pacifism, Zionism, A-bomb
See virtual exhibit, “Einstein’s Revolution,” AmericanMuseum of Natural History (www.amnh.org/exhibitions/einstein/revolution/index.php)
The first 1905 paper“On a heuristic viewpoint regarding the
production and transformation of light”(the light quanta paper)
Applied old theory (Planck’s) to old data (Hertz’sphotoelectric effect)
Heuristic = aid to solving a problem, not otherwisejustifiable (makes light quantized particle, not wave)
Controversial challenge to wave theory, not widelyaccepted until 1915 (earns Nobel Prize, 1921)
Frequency of light
E of
ele
ctro
nThreshold
metal
Light Electrons
The second 1905 paperBrownian motion
– Old theory (heat is motion) applied to old data(botanist Robert Brown’s “jumping” pollenparticles, 1827)
– Used statistics to derive atomic parametersfrom measurements of visible motions ofparticles
– Proved existence of atoms (contra Mach’s“positivism”)
Asks simple, yet profound questions
The third 1905 paper (SR) Theory of measurement and how we know,
not a theory about nature Not general relativity (later, 1907-16) Continues style of asking simple, profound
questions Contributions from Mileva Maric?
– “When you’re my dear little wife we’ll diligently workon science together so we won’t become old philistines,right?” Einstein to Maric, 1901
Newton’s implicit theory ofmeasurement
Abolute time and space Instantaneous communicationVelocities addGalileo’s ‘principle of relativity’ (same
physics in inertial reference frames)
Vtrain
vball
Vball = Vtrain + vball
Sue
Joe
“Aether drift” problem, 1880s(do light velocities add?)
Ve = 3 x 104 m/s
c = 3 x 108 m/s
VJan measured = c + Ve?
VJun-measured = c - Ve?
Assume aetherfixed wrt stars
Two ad-hoc solutions to measured “null” result--Earth drags aether around sun?--Length contraction against aether wind?
Sun
Jan
Jun
(longer ruler?)
(shorter ruler?)
Einstein’s “Electrodynamcisof Moving Bodies” (1905) Asymmetries in Maxwell equations
no absolute rest with with respect to an aether
Begins with two postulates I. Principle of relativity
Physics invariant in inertial reference frames
II. Invariance of speed of light Predicted by Maxwell’s equations
Einstein calls theory the “invariance of light” Planck coined term “relativity” in 1906
Consequences of 2 postulatesElectrodynamics without an aetherNew theory of measurement because
simultaneity becomes relative– Simultaneous = Same time and same place– Arrival of train at 7 means “the pointing of the
small hand on my watch to 7 and the arrival ofthe train [beside me] are simultaneous events”
Moving clocks, lengths, masses change!Holds only for inertial motion (General
Relativity is for accelerated motion)
Relativity of simultaneity
Simultaneity always relative to reference frame!
Thunderbolt 1 Thunderbolt 2
Joe fixed on the landscape (1, 2 same time)
Sue moving on train (first 2, then 1)
Mirrors
Start Later
Time dilation (moving clocksslow down)
VStationary clock, Ts Moving clock, Tm
d
Time = Distance/VelocityTs = 2d/c
Tick
Tock
Let Ts = 1 secIf V = 0.6c, Tm = 1.3 secIf V = 0.8c, Tm = 1.7 secIf V = 0.99c, Tm = 7.1 sec
d
Mirror
!
Tm =Ts
1" v2/c
2
Some algebra yields:
Moving lengths contract
Tick
Tock
V
Stationary length
Movinglength
Ls
Lm
… and moving masses increase:
!
Mm =Ms
1" v2/c
2
!
Lm = Ls 1" v2/c
2 … a little algebra yields:
More consequences of SR E = mc2
“Events” happen in a given place at agiven time (“spacetime”)
Light beamt
xPast
FutureNow
One-Dimensional Spacetime (Minkowski)
“My future”