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Chapter 1. The principle of relativity

Chapter 1. The principle of relativity. Section 1. Velocity of propagation of interaction. To describe processes, we need coordinates and clocks. These define a “system of reference.”.

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Chapter 1. The principle of relativity

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  1. Chapter 1. The principle of relativity Section 1. Velocity of propagation of interaction

  2. To describe processes, we need coordinates and clocks • These define a “system of reference.”

  3. If a free body (Fext = 0) moves at constant velocity v in a particular reference system K, then K is an inertial reference system. K V

  4. If a reference system K’ moves uniformly relative to an inertial reference system K, then K’ is inertial, too. K’ K V

  5. Principle of relativity: All laws of nature are identical in all inertial reference systems (experiment!) The equations expressing laws are invariant (same form) under transformation of coordinates and time.

  6. Newtonian Mechanics: Interactions are described by potential energy. This assumes instantaneous propagation. • If the source of an electric force moves or changes, a test charge feels it with no delay - F

  7. Experiment: There always is a delay. • Velocity of propagation is finite. • If finite, it must have a maximum value. • A consequence is that motion of particles cannot exceed this maximum. • Maximum is called the “signal velocity.”

  8. Signal velocity must be the same in all inertial reference systems. By principle of relativity, if there is a maximum propagation velocity in one inertial reference system K, it must have the same value in any other inertial reference system K’. Signal velocity is a universal constant = “c”.

  9. Principle of relativity + finite signal velocity = Principle of relativity of Einstein • Relativistic Mechanics

  10. The transition from relativistic to classical mechanics is effected in formulas by setting • c -> 0 • c -> infinity • c-> 2.998 x 1010 cm/s 1 2 3

  11. The transition from relativistic to classical mechanics is effected in formulas by setting • c -> 0 • c -> infinity • c-> 2.998 x 1010 cm/s

  12. Distance is already relative in classical mechanics. • Spatial relations depend on reference system. • Two non-simultaneous events can occur at the same place or at different places depending on the system. K’ K V

  13. Time is absolute in classical mechanics. • The interval of time between two events is the same in all systems. • Velocity of composite motion = vector sum of individual velocities. • This universal law of classical mechanics if applied to propagation of interactions would mean the signal velocity should depend on the reference system. • Contradicts Einstein relativity principle. • This is confirmed by Michelson experiment: No dependence of light velocity on direction of earth’s motion.

  14. Time cannot be absolute in relativisitic mechanics. • Events simultaneous in one system K’ will not be in a different system K. K’ K V

  15. Two inertial reference systems, K’ moves relative to K along X (X’). • Two signals start from A simultaneously. • Both signals travel at c. • They reach points B and C, equidistant from A, simultaneously in K’. Z’ Z V B A C K’ X’ K X Y’ Y

  16. The two events, which are simultaneous in K’, are not simultaneous in K. • In K, both signals also travel at c. • But B moves towards source while C moves away. • Signal arrives at B earlier than at C in K system. Z’ Z V B A C K’ X’ K X Y’ Y

  17. An “EVENT” occurring in a material particle is defined by 3 spatial coordinates of the particle and the time of the occurrence. • The time of occurrence is different in different inertial reference systems, and is not absolute. • Events are “WORLD POINTS” in 4-dimensional space with x,y,z,t axes.

  18. Which statement is not true? • All physical laws have the same form in all inertial reference systems. • The maximum possible signal velocity is the same in all reference systems. • The signal velocity depends on the motion of the observer. 1 2 3

  19. Which statement is not true? • All physical laws have the same form in all inertial reference systems. • The maximum possible signal velocity is the same in all reference systems. • The signal velocity depends on the motion of the observer.

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