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Time, clocks and the speed of light

Time, clocks and the speed of light. Vasco Guerra and Rodrigo de Abreu Departamendo de Física, Instituto Superior Técnico, 1049-001 Lisboa, Portugal email contact: vguerra@alfa.ist.utl.pt. The Michelson-Morley experiment. Time and clocks. Time: is what is measured with clocks. Clocks:

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Time, clocks and the speed of light

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  1. Time, clocks and the speed of light Vasco Guerra and Rodrigo de Abreu Departamendo de Física, Instituto Superior Técnico, 1049-001 Lisboa, Portugal email contact: vguerra@alfa.ist.utl.pt

  2. The Michelson-Morley experiment

  3. Time and clocks • Time: • is what is measured with clocks. • Clocks: • any periodic phenomenon may be associated with a clock (in principle...). • The “rest system”: • “A coordinate system in which Newton’s equations are valid”. • A coordinate system in which the speed of light in vacuum is c.

  4. Feynman’s light clock

  5. The “first” assumption • Time passes independently from the type of clocks used to measure it. • Time measurements of a certain clock do not depend on its orientation!

  6. The “second” assumption • Clocks measure time in the same way in different inertial “moving” frames. • The notion of time is the same in all inertial frames. ... is true for any “moving” inertial system as well!

  7. Two Feynman light clocks ... is true for any “moving” inertial system as well! • In each inertial frame the two-way speed of light is “constant”.

  8. Two Feynman-like bullet clocks • In each inertial frame the two-way speed of bullets is “constant”.

  9. “Constancy” of speed • In each frame the two-way speed is the same (“constant”) in all directions.  Both for light and for bullets! • In allframes the two-way speed is the same (“constant”) in all directions. • In each frame the speed is the same (“constant”) independently of thespeed of the source.

  10. “Constancy” in all frames • Feynman clock with bullets in a train (S’): • The two-way speed of bullets fired in a “moving” train is different if measured in the train or in the station: the same bullets travel with different speeds in different frames. • The same Feynman clock with bullets in the station (S): • Is the two-way speed of bullets fired in the station (“rest system”) the same as before? In S’: x’=v’t’ In S: x=vt x: total distance in the round trip v: two-way speed • v=v’

  11. “Constancy” in all frames (continued) • The two-way speed of bullets is the same (“constant”) in all frames: different bullets travel with the same two-way speedin all frames  Both for light and for bullets! • The constancy of the two-way speed in all frames refers to different objects!

  12. The “third” assumption • There exists a limit speed in the “rest system”: no object can travel in the rest system with a speed higher than a certain value c. • Objects moving with the limit speed in the rest system must do so independently of the speed of the emitting source.

  13. The “third” assumption (continued) • Different objects, emitted from different inertial frames, collapse into the same object if (and only if) they travel with the (two-way) limit speed c. • Light travels with the limit speed in the “rest system”. • The distinction between “two” light rays is artificial. • The same light rays travel with the same two-way speed in all inertial frames.

  14. Conclusions The null result of the Michelson-Morley experiment and the constancy of the two-way speed of light in vacuum are deeply connected with the very notion of time. • All good clocks can be used to measure time, independently from the machinery involved in their manufacturing. • Time is measured in the same way in all inertial frames. • A limit speed exists in the “rest system”.

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