Chapter S2: Space and Time

 

Introduction
         Einstein
         1905: Special Theory of Relativity -> Space and Time
         1915: General Theory of Relativity -> Space, Time, and Gravity
         This chapter is about the Special Theory of Relativity

Reference Frames
        
         Earth Example of motion relative to different reference frames
         Example of motion in a straight line
        
         This chapter deals with reference frames having constant velocity
                  (no acceleration)
         "Constant velocity reference frame" = "free float frame"
                  = "inertial reference frame"
        

Underlying "assumptions" of Special Relativity
        
         1.) The laws of physics work just as well in any reference frame as in any other
         2.) The speed of light seems to be the same, no matter what reference frame
                  you are in
         i.e. If light is produced in a different reference frame (moving at velocity = v1),
                  you, in your frame, don't see light's velocity as c + v1,
                  you see light's velocity as c!
                 
                  1887, Michelson Morley Experiment
                  Binary stars example
                  Car example
                  Colliding cars are equivalent to colliding galaxies
                  (NGC 5426 & 5427 and NGC 4038 & 4039
                  and we don't see crumpled galaxies waiting to be hit!)

                                           

Clarifications
         To notice the effects of relativity, you need very fast motions

         Slow objects act in ways we are familiar with (Example)
         But light doesn't (Example)

         We assume that the light is traveling through a vacuum
                  (not glass, etc.)

Ramifications:
Time Dilation:
         Jackie => moving reference frame
         Everyday, non-relativistic experience with a ball:
                  Ball example
                  Ball's path is longer path in viewer's frame than in
                  thrower's frame

         Same geometry, but using light rather than a ball:
                  Light Example
                  You still see a longer path than Jackie does
                  Light moves at same speed in all inertial reference frames
                  time = distance / velocity
                  Therefore, you measure a longer time than Jackie does

         Note: test with "pi+" meson traveling at fast speed.
                  Slowed the decay time in our reference frame
                  (which, to the pi+ meson, is moving)

         Note: in 1975 someone tested this by putting a clock on an airplane.
                  After 15 hours in flight, the on-board clock was 6 nanoseconds
                  behind the Earth clocks

 

Length contraction:
         Figure

Loss of Simultaneity:
         Train example

Mass Dilation:
         Figure

Velocity Addition:
         Figure

 

Summary of Important Ramifications:
         1.) Time runs slower in a moving object's reference frame
         2.) If you look at a moving object, it looks shorter to you
                  (and you look shorter to it)
         3.) If you look at a moving object, it seems more massive to you
                  (and you look more massive to it)
         4.) Two events that are simultaneous in one reference frame
                  are not simultaneous in other inertial reference frames
         5.) Nothing can move faster than the speed of light

 

Other:
         Twin paradox