1. Chapter 37 Special Relativity
The postulates
Events and frames
The relativity of simultaneity, time and length
The Lorentz transformation
The relativity of velocities
The Doppler effect of light
A new look at momentum and energy

2. Validity of Maxwell’s equations
The postulates:
Validity of Maxwell’s equations
The Michelson-Morley experiment

3. The speed of light in vacuum has been defined to be exactly
The postulates, The Ultimate Speed:
The speed of light in vacuum has been defined to be exactly
c = m/s.
It is found to be the ultimate speed.

4. Measuring an Event:
An event is something that happens, and every event can be assigned three space coordinates and one time coordinate.
The Space Coordinates. We imagine the observer’s coordinate system fitted with a close-packed, three-dimensional array of measuring rods, one set of rods parallel to each of the three coordinate axes. These rods provide a way to determine coordinates along the axes.
The Time Coordinate. For the time coordinate, we imagine that every point of intersection in the array of measuring rods includes a tiny clock, which the observer can read because the clock is illuminated by the light generated by the event.
The Spacetime Coordinates. The observer can now assign spacetime coordinates to an event by simply recording the time on the clock nearest the event and the position as measured on the nearest measuring rods. If there are two events, the observer computes their separation in time as the difference in the times on clocks near each and their separation in space from the differences in coordinates on rods near each.

5. # Synchronization of all clocks is needed and achievable.
Measuring an Event:
# Synchronization of all clocks is needed and achievable.

6. The Relativity of Simultaneity:

7. The Relativity of Simultaneity, A Closer Look:
Fig The spaceships of Sally and Sam and the occurrences of events from Sam’s view. Sally’s ship moves rightward with velocity, v . (a) Event Red occurs at positions
RR’ and event Blue occurs at positions BB’; each event sends out a wave of light. (b) Sam simultaneously detects the waves from event Red and event Blue. (c) Sally detects the wave from event Red. (d) Sally detects the wave from event Blue. With the postulate of constant speed of light, Sally would say event Red happens earlier.

8. The Relativity of Time:

9. The Relativity of Time:
In the previous case, Sally measures a proper time interval, and Sam measures a greater time interval. The amount by which a measured time interval is greater than the corresponding proper time interval is called time dilation.
g is called the Lorentz factor.

10. Example, Time dilation of spacecraft which returns to Earth:

11. Example, Time dilation and travel distance for a relativistic particle:

12. The Relativity of Length:

13. The Relativity of Length, Proof:
Consider that both Sally, seated on a train moving through a station, and Sam, again on the station platform, want to measure the length of the platform.
Sam, using a tape measure, finds the length to be L0, a proper length, because the platform is at rest with respect to him. Sam also notes that Sally, on the train, moves through this length in a time Dt =L0/v, where v is the speed of the train.
Therefore,
For Sally, however, the platform is moving past her. She can measure the ends of the platform at the same place in her reference frame. She can time them with a single stationary clock, and so the interval Δt0 that she measures is a proper time interval. To her, the length L of the platform is given by
Therefore, and finally,

14. The Relativity of Length:
Let L0 be the length of a rod that you measure when the rod is stationary (meaning you and it are in the same reference frame, the rod’s rest frame). If, instead, there is relative motion at speed v between you and the rod along the length of the rod, then with simultaneous measurements you obtain a length L given by
Since the Lorentz factor g is always greater than unity if there is relative motion, L is less than L0.

15. Example, Time dilation and length contraction:

16. Example, Time dilation and length contraction as seen in outrunning a supernova :

17. The Galilean Transformation:

18. Based on the constancy of the speed of light in all inertial frames
The Lorentz Transformation Equations:
Based on the constancy of the speed of light in all inertial frames
The Lorentz transformation equations are:
(The equations are written with the assumption that t =t’= 0 when the origins of S and S’ coincide.)

19. The Lorentz Transformation Equations:

20. Some Consequences of Lorentz Transformation Equations:
Simultaneity:

21. Some Consequences of Lorentz Transformation Equations:
Time Dilation:

22. Some Consequences of Lorentz Transformation Equations:
Length Contraction:

23. Example, Time dilation and reversing the sequence of events:
Note: the distance measured from the ship’s frame is based on the burst and explosion events, not measurements at the same time. The ship is not necessary at the origin, or, the moon and planet may better be drawn at the negative X-axis.

24. Example, Time dilation and reversing the sequence of events, cont.:

25. The Relativity of Velocities:

26. The Doppler effect of light in general:

27. The Doppler Effect of Light:
The Doppler effect is a shift in detected frequency for traveling waves.
The Doppler effect for light waves depends on only one velocity, the relative velocity, v, between source and detector, as measured from the reference frame of either.
Let f0 represent the proper frequency of the source—that is, the frequency that is measured by an observer in the rest frame of the source. Let f represent the frequency detected by an observer moving with velocity relative to that rest frame.
Then, when the direction of is directly away from the source radially,
For low speeds (b « 1), this equation can be expanded in a power series in b and approximated as

28. # Red shift and blue shift
The Doppler Effect of Light, Astronomical Effect:
# Red shift and blue shift

29. The Doppler effect of light in general:
The Doppler Effect of Light, Transverse Doppler Effect:
The transverse Doppler effect.
In terms of period of oscillations,
Where To is the proper period.
The Doppler effect of light in general:

30. A New Look at Momentum:
(The motivation to do so is to look for a four vector.)
# Momentum, with the definition p =mv, does not transform like a vector.
# Concept of four vectors, space-time four vector, proper time as a scalar

31. For v << c A New Look at Energy, Kinetic Energy:
(The time component of
the energy-momentum four vector)
For v << c

32. X 299 792 458 m/s 閒談狹義相對論與廣義相對論： 四維時空，質能互換 光速恆定的假設 伽利略 時空座標轉換 勞倫茲

33. 閒談狹義相對論與廣義相對論：
四維時空，質能互換
時空位置四向量
能量動量四向量

34. 牛頓力學
狹義相對論

35. A New Look at Energy, Momentum and Kinetic Energy:

36. A New Look at Energy, Mass Energy:
An object’s mass m and the equivalent energy E0 are related by:
This energy that is associated with the mass of an object is called mass energy or rest
energy.
Masses are usually measured in atomic mass units, where
1 u = kg,
and energies are usually measured in electron-volts or multiples of it, where
1 eV= J.

37. A New Look at Energy, Total Energy:
In a system undergoing a chemical or nuclear reaction, a change in the total mass energy of the system due to the reaction is often given as a Q value. The Q value for a reaction is obtained from the relation

38. Example, Energy and momentum of a relativistic electron:

39. Example, Energy and discrepancy in travel time:

40. The postulates
Events and frames
The relativity of simultaneity, time and length
The Lorentz transformation
The relativity of velocities
The Doppler effect of light
A new look at momentum and energy