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This is how we would measure a
cartwheel in the few moments it passes by us at 87% of of the speed of
light. At axle height, the wheel appears Lorentz-contracted by a factor
of 2 along the direction of motion. The bottom of the cartwheel, where it
touches the road, is not moving, and is not Lorentz-contracted. You might
think that the top of the cartwheel would have to move faster than the speed
of light to overtake the axle moving at 87% of the speed of light; but of
course it can't (remember how to add velocities!). The cartwheel is also an example of the impossibility of completely rigid bodies in special relativity. The rim is Lorentz-contracted, but the spokes have their full length when vertical - they must bend and compress, otherwise they could be used to transmit a signal faster than the speed of light.
Lectures 9, 10 - refer to the Reading belowThe most precise blackbody in nature is the whole universe, filled with blackbody radiation at a temperature of 2.7 K. See how well the curve fits the data in this brief Cosmology Tutorial by Ned Wright at UCLA.
Also read Krane section 3.6 on "What is a photon?" Here is what Albert Einstein had to say: ``All the fifty years of conscious brooding have brought me no closer to the answer to the question, "what are light quanta?" Of course today every rascal thinks he knows the answer, but he is deluding himself.''
Some examples of atomic emission lines arising from quantized energy level transitions: