1. Physics 1161: Lecture 26
Special Relativity
Sections 29-1 – 29-6

2. Special Relativity

3. Null result of Michelson Morley Experiment
Relative motion of magnet and loop of wire induces current in loop

4. Michelson-Morley Experiment
Null Result
Designed to prove the existence of the ether – the still reference frame
Speed of light was the same no matter the direction relative to the earth’s motion
Interferometer

5. 3 mph eastward 3 mph westward 57 mph eastward 57 mph westward
You and your friend are playing catch in a train moving at 60 mph in an eastward direction. Your friend is at the front of the car and throws you the ball at 3 mph (according to you). What velocity does the ball have when you catch it, according to you?
3 mph eastward
3 mph westward
57 mph eastward
57 mph westward
60 mph eastward

6. 3 mph eastward 3 mph westward 57 mph eastward 57 mph westward
You and your friend are playing catch in a train moving at 60 mph in an eastward direction. Your friend is at the front of the car and throws you the ball at 3 mph (according to you). What velocity does the ball have when you catch it, according to you?
3 mph eastward
3 mph westward
57 mph eastward
57 mph westward
60 mph eastward

7. 63 mph eastward 63 mph westward 57 mph eastward 57 mph westward
You and your friend are playing catch in a train moving at 60 mph in an eastward direction. Your friend is at the front of the car and throws you the ball at 3 mph (according to you). What velocity does the ball have as measured by someone at rest on the platform?
63 mph eastward
63 mph westward
57 mph eastward
57 mph westward
60 mph eastward

8. 63 mph eastward 63 mph westward 57 mph eastward 57 mph westward
You and your friend are playing catch in a train moving at 60 mph in an eastward direction. Your friend is at the front of the car and throws you the ball at 3 mph (according to you). What velocity does the ball have as measured by someone at rest on the platform?
63 mph eastward
63 mph westward
57 mph eastward
57 mph westward
60 mph eastward

9. Inertial Reference Frame
Frame in which Newton’s Laws Work
Moving is OK but….
No Accelerating
No Rotating
Technically Earth is not inertial, but it’s close enough.
Small distance gives quantum mechanics. High speed gives relativity

10. Which of the following systems are not inertial reference frames?
a person standing still
an airplane in mid-flight
a merry-go-round rotating at a constant rate
all of the above are IRFs
none of the above are IRFs

11. Which of the following systems are not inertial reference frames?
a person standing still
an airplane in mid-flight
a merry-go-round rotating at a constant rate
all of the above are IRFs
none of the above are IRFs
An inertial reference frame is the same as a non-accelerating reference frame. Due to the circular motion of the merry-go-round, there is a centripetal acceleration, which means that the system is accelerating. Therefore it is not an inertial reference frame.

12. Special Theory of Relativity Postulates
All laws of nature are the same in all uniformly moving frames of reference.
The speed of light in free space has the same measured value for all observers, regardless of the motion of the source or the motion of the observer; that is, the speed of light is a constant.
The speed of a light flash emitted by the space station is measured to be c by observers on both the space station and the rocket ship.

13. Which of these quantities change when you change your reference frame?
position
velocity
acceleration
All of the above
Only a) and b)

14. Which of these quantities change when you change your reference frame?
position
velocity
acceleration
All of the above
Only a) and b)
Position depends on your reference frame – it also depends on your coordinate system. Velocity depends on the difference in position, which also relates to the frame of reference. However, since acceleration relates to the difference in velocity, this will actually be the same in all reference frames.

15. Simultaneity
two events are simultaneous if they occur at the same time.
From the point of view of the observer who travels with the compartment, light from the source travels equal distances to both ends of the compartment and therefore strikes both ends simultaneously.

16. Simultaneity

17. Simultaneity
Two events that are simultaneous in one frame of reference need not be simultaneous in a frame moving relative to the first frame.
Because of the ship's motion, light that strikes the back of the compartment doesn't have as far to go and strikes sooner than light strikes the front of the compartment.

18. A boxcar moves to the right at a very high speed
A boxcar moves to the right at a very high speed. A green flash of light moves from right to left, and a blue flash from left to right. For someone with sophisticated measuring equipment in the boxcar, which flash takes longer to go from one end to the other? v
the blue flash
the green flash
both the same

19. A boxcar moves to the right at a very high speed
A boxcar moves to the right at a very high speed. A green flash of light moves from right to left, and a blue flash from left to right. For someone with sophisticated measuring equipment in the boxcar, which flash takes longer to go from one end to the other? v
the blue flash
the green flash
both the same
The speed of light is c inside the boxcar, and the distance that each flash must travel is L (length of boxcar). So each flash will take t = L/c, which will be the same for each one.

20. A boxcar moves to the right at a very high speed
A boxcar moves to the right at a very high speed. A green flash of light moves from right to left, and a blue flash from left to right. According to an observer on the ground, which flash takes longer to go from one end to the other? v
the blue flash
the green flash
both the same

21. A boxcar moves to the right at a very high speed
A boxcar moves to the right at a very high speed. A green flash of light moves from right to left, and a blue flash from left to right. According to an observer on the ground, which flash takes longer to go from one end to the other? v
the blue flash
the green flash
both the same
The ground observer still sees the light moving at speed c. But while the light is going, the boxcar has actually advanced. The back wall is moving toward the blue flash, and the front wall is moving away from the green flash. Thus, the green flash has a longer distance to travel and takes a longer time.

22. Time Dilation

23. Time Dilation D
t0 is proper time
Because it is rest frame of event

24. Time Dilation L=v Dt D D ½ vDt t0 is proper time
Because it is rest frame of event

25. no pulse - the astronaut died a long time ago
An astronaut moves away from Earth at close to the speed of light. How would an observer on Earth measure the astronaut’s pulse rate?
it would be faster
it would be slower
it wouldn’t change
no pulse - the astronaut died a long time ago

26. no pulse - the astronaut died a long time ago
An astronaut moves away from Earth at close to the speed of light. How would an observer on Earth measure the astronaut’s pulse rate?
it would be faster
it would be slower
it wouldn’t change
no pulse - the astronaut died a long time ago
The astronaut’s pulse would function like a clock. Since time moves slower in a moving reference frame, the observer on Earth would measure a slower pulse.

27. Less than 2 seconds 2 seconds More than 2 seconds
The period of a pendulum attached in a spaceship is 2 seconds while the spaceship is parked on Earth. What is its period for an observer on Earth when the spaceship moves at 0.6c with respect to Earth?
Less than 2 seconds
2 seconds
More than 2 seconds

28. Less than 2 seconds 2 seconds More than 2 seconds
The period of a pendulum attached in a spaceship is 2 seconds while the spaceship is parked on Earth. What is its period for an observer on Earth when the spaceship moves at 0.6c with respect to Earth?
Less than 2 seconds
2 seconds
More than 2 seconds
To the Earth observer, the pendulum is moving relative to him and so it takes longer to swing (moving clocks run slow) due to the effect of time dilation.

29. Less than 2 seconds 2 seconds More than 2 seconds
The period of a pendulum attached in a spaceship is 2 seconds while the spaceship is parked on Earth. What would the astronaut in the spaceship measure the period to be?
Less than 2 seconds
2 seconds
More than 2 seconds

30. Less than 2 seconds 2 seconds More than 2 seconds
The period of a pendulum attached in a spaceship is 2 seconds while the spaceship is parked on Earth. What would the astronaut in the spaceship measure the period to be?
Less than 2 seconds
2 seconds
More than 2 seconds

31. Space Travel
Example
Alpha Centauri is 4.3 light-years from earth. (It takes light 4.3 years to travel from earth to Alpha Centauri). How long would people on earth think it takes for a spaceship traveling v=0.95c to reach A.C.?
How long do people on the ship think it takes?

32. Space Travel
Example
Alpha Centauri is 4.3 light-years from earth. (It takes light 4.3 years to travel from earth to Alpha Centauri). How long would people on earth think it takes for a spaceship traveling v=0.95c to reach A.C.?
How long do people on the ship think it takes?
People on ship have ‘proper’ time they see earth leave, and Alpha Centauri arrive. Dt0
Dt0 = 1.4 years
Physics 1161: Lecture 28, Slide 32

33. Length Contraction Example
People on ship and on earth agree on relative velocity v = 0.95 c. But they disagree on the time (4.5 vs 1.4 years). What about the distance between the planets?
Earth/Alpha d0 = v t
Ship d = v t
Length in moving frame
Length in object’s rest frame

34. Length Contraction Example
Sue is carrying a pole 10 meters long. Paul is on a barn which is 8 meters long. If Sue runs quickly v=.8 c, can she ever have the entire pole in the barn?
Paul:
Sue:

35. Length Contraction Example
People on ship and on earth agree on relative velocity v = 0.95 c. But they disagree on the time (4.5 vs 1.4 years). What about the distance between the planets?
Earth/Alpha d0 = v t
= .95 (3x108 m/s) (4.5 years)
= 4x1016m (4.3 light years)
Ship d = v t
= .95 (3x108 m/s) (1.4 years)
= 1.25x1016m (1.3 light years)
Length in moving frame
Length in object’s rest frame
Physics 1161: Lecture 28, Slide 35

36. Length Contraction Gifs
v=0.1 c
v=0.8 c
v=0.95 c

37. Your spaceship is parked outside an interstellar cafe
Your spaceship is parked outside an interstellar cafe. A speeder zooms by in an identical ship traveling at half the speed of light. From your perspective, their ship looks:
Longer than your ship
Shorter than your ship
Exactly the same as your ship

38. Exactly the same as your ship
Your spaceship is parked outside an interstellar cafe. A speeder zooms by in an identical ship traveling at half the speed of light. From your perspective, their ship looks:
Longer than your ship
Shorter than your ship
Exactly the same as your ship
Lo > L
In the speeder’s reference frame
In your reference frame
Always <1

39. Comparison: Time Dilation vs. Length Contraction
Dto = time in same reference frame as event
i.e. if event is clock ticking, then Dto is in the reference frame of the clock (even if the clock is in a moving spaceship).
Lo = length in same reference frame as object
length of the object when you don’t think it’s moving.
Dt > Dto
Time seems longer
from “outside”
Lo > L
Length seems shorter
from “outside”

40. Relativistic Momentum
Note: for v<<c p=mv
Note: for v=c p=infinity
Relativistic Energy
Note: for v=0 E = mc2
Note: for v<<c E = mc2 + ½ mv2
Note: for v=c E = infinity (if m<> 0)
Objects with mass can’t go faster than c!

41. Summary Physics works in any inertial frame
Simultaneous depends on frame
Proper frame is where event is at same place, or object is not moving.
Time dilates
Length contracts
Energy/Momentum conserved
For v<<c reduce to Newton’s Laws