1 / 60

Kinematical Relations in Special Relativity: Gedanken Experiments

This lecture explores four thought experiments that demonstrate the kinematical relations in special relativity, including length contraction, time dilation, and clock synchronization.

backermann
Download Presentation

Kinematical Relations in Special Relativity: Gedanken Experiments

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Lecture Six

  2. Kinematical RelationsinSpecial Relativity

  3. adapted from …

  4. Four Gedanken Experimente“thought experiments”thought 是由過去分詞轉變而成的分詞形容詞不是名詞正譯:想像實驗誤譯:思想實驗

  5. Experiment I Comparison of parallel measuring sticks oriented perpendicular to their direction of motion

  6. Experiment II Comparison of clock rates

  7. Experiment III Comparison of lengths parallel to the direction of motion

  8. Experiment IV The synchronization of clocks

  9. Experiment I Comparison of parallel measuring sticks oriented perpendicular to their direction of motion (invariance of perpendicular length)

  10. Experiment II Comparison of clock rates (time dilation)

  11.  t'being measured by a single clock is a proper time

  12. Frequently used symbols in special relativityexcept

  13. Experiment III Comparison of lengths parallel to the direction of motion (length contraction)

  14. Two Derivations of Length Contraction • Simple derivation • Detailed derivation

  15. Simple Derivation For observer on the station (S): The time of passage t0 is a proper time, the length L of the train is not a proper length.

  16. Simple Derivation For observer on the train (S ): The time of passage t is not a proper time, the length L0 of the train is a proper length.

  17. Simple Derivation

  18. Detailed Derivation

  19. train station

  20. Experiment III For train observer:  t'is a proper time interval, being observable with a single clock  t' = 2L' /c

  21. Experiment III For station observer:  t is not a proper time interval, being measured between two points with two clocks  t =  t1+  t 2

  22. Experiment III  t1:light signal from B0 to M1  t2 :light signal from M1 to B2

  23. Experiment III c t1= B0 M1 = B0 B1+ B1 M1 = v t1+ L c  t2 = M1 B2 = M1 B1-B1 B2 = L- v t2

  24.  t' is a proper time interval, being observable with a single clock  t' = 2L' /c

  25. Summary • Proper time: time interval measured by a single clock • Proper length: length measured by an observer stationary relative to the observed.

  26. Summary Length Contraction The length of a moving stick is shortened by a factor of

  27. Summary L0 : proper length of a stick L : length of this stick in motion

  28. Summary Time Dilation A moving clock runs slow by a factor of

  29. Summary  t0 : time interval measured in a clock  t : time interval measured in a frame in which this clock is moving

  30. Experiment IV The Synchronization of Clocks The phase difference in the Synchronization of Clocks

  31. Two stationary clocks A and B synchronized and separated by proper distance L' in S'-frame

  32. Single clock S in a stationary in S-frame

  33. By comparing S with A and B, observer in S claims that A and B are not synchronized.

  34. Event EA: clock in  meets clock A. Event EB: clock in  meets clock B. Times in : tA = t0, tB = t1 (proper time) Times in ' : t'A = t'0, t'B = t'1

  35. t' = t'B -t'A • t = tB -tA

  36.  t = tB – tA is the time interval measured by a single clock in proper time

  37. For an observer in , the time interval on both of the ' clocks individually would appear too large by the same time dilation factor, but they will not be in time with each other to a single observer in .

  38. The leading clock at A lags the trailing clock at B by 

  39. The leading clock at A lags the trailing clock at B by 

More Related