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Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6
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Page 1: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

Special RelativityPhysics 1161: Lecture 35

Sections 29-1 – 29-6

Page 2: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

Special Relativity

Page 3: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

• Null result of Michelson Morley Experiment• Relative motion of magnet and loop of wire

induces current in loop• http://www.fourmilab.ch/etexts/einstein/spec

rel/www/

Page 4: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

Michelson-Morley Experiment

Inte

rfer

omet

er

• 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

Null Result

Page 5: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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?

1) 2) 3) 4) 5)

0% 0% 0%0%0%

1) 3 mph eastward2) 3 mph westward3) 57 mph eastward4) 57 mph westward5) 60 mph eastward

Page 6: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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?

1) 2) 3) 4) 5)

0% 0% 0%0%0%

1) 3 mph eastward2) 3 mph westward3) 57 mph eastward4) 57 mph westward5) 60 mph eastward

Page 7: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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?

1) 2) 3) 4) 5)

0% 0% 0%0%0%

1) 63 mph eastward2) 63 mph westward3) 57 mph eastward4) 57 mph westward5) 60 mph eastward

Page 8: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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?

1) 2) 3) 4) 5)

0% 0% 0%0%0%

1) 63 mph eastward2) 63 mph westward3) 57 mph eastward4) 57 mph westward5) 60 mph eastward

Page 9: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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.

Page 10: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

Which of the following systems are not inertial reference frames?

1) 2) 3) 4) 5)

0% 0% 0%0%0%

1) a person standing still 2) an airplane in mid-flight 3) a merry-go-round rotating

at a constant rate4) all of the above are IRFs 5) none of the above are IRFs

Page 11: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

Which of the following systems are not inertial reference frames?

1) 2) 3) 4) 5)

0% 0% 0%0%0%

1) a person standing still 2) an airplane in mid-flight 3) a merry-go-round rotating

at a constant rate4) all of the above are IRFs 5) 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.

Page 12: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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.

Page 13: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

Which of these quantities change when you change your reference frame?

1) 2) 3) 4) 5)

0% 0% 0%0%0%

1) position2) velocity3) acceleration4) All of the above5) Only a) and b)

Page 14: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

Which of these quantities change when you change your reference frame?

1) 2) 3) 4) 5)

0% 0% 0%0%0%

1) position2) velocity3) acceleration4) All of the above5) 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.

Page 15: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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.

Page 16: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

Simultaneity

• http://sq.netlog.com/go/explore/videos/videoid=sq-18174

Page 17: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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.

Page 18: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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?

1) 2) 3)

0% 0%0%

1) the blue flash2) the green flash3) both the same v

Page 19: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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?

1) 2) 3)

0% 0%0%

1) the blue flash2) the green flash3) both the same v

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.

Page 20: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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?

1) 2) 3)

0% 0%0%

1) the blue flash2) the green flash3) both the same v

Page 21: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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?

1) 2) 3)

0% 0%0%

1) the blue flash2) the green flash3) both the same

v

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.

Page 22: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

Time Dilation

• http://www.youtube.com/watch?v=KHjpBjgIMVk&feature=related

Page 23: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

Time Dilation

D

Dtc 20

cD

t2

0

t0 is proper time

Because it is rest frame of event

Page 24: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

Time Dilation

D D

L=v Dt

Dtc 20

cD

t2

0

22

22

tv

Dtc

2

2

1

12

cvc

Dt

2

20

1cv

tt

½ vDt

t0 is proper time

Because it is rest frame of event

Page 25: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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?

1) 2) 3) 4)

0% 0%0%0%

1) it would be faster2) it would be slower3) it wouldn’t change4) no pulse - the astronaut

died a long time ago

Page 26: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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?

1) 2) 3) 4)

0% 0%0%0%

1) it would be faster2) it would be slower3) it wouldn’t change4) 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.

Page 27: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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?

1) 2) 3)

0% 0%0%

1) Less than 2 seconds2) 2 seconds3) More than 2 seconds

Page 28: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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?

1) 2) 3)

0% 0%0%

1) Less than 2 seconds2) 2 seconds3) 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.

Page 29: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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?

1) 2) 3)

0% 0%0%

1) Less than 2 seconds2) 2 seconds3) More than 2 seconds

Page 30: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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?

1) 2) 3)

0% 0%0%

1) Less than 2 seconds2) 2 seconds3) More than 2 seconds

Page 31: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

Space TravelAlpha 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?

Page 32: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

Physics 1161: Lecture 28, Slide 32

Space TravelAlpha 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.?

vd

t c 95.0years-light 3.4 years 5.4

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

2

20

1cv

tt

2

2

0 1cv

tt 295.15.4

Dt0 = 1.4 years

Page 33: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

Length Contraction

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

2

2

0 1cv

LL

Length in moving frame

Length in object’s rest frame

Page 34: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

Length ContractionSue 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:

2

2

0 1cv

LL

Sue:

2

2

0 1cv

LL

Page 35: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

Physics 1161: Lecture 28, Slide 35

Length Contraction

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)

2

2

0 1cv

LL

Length in moving frame

Length in object’s rest frame

Page 36: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

Length Contraction Gifs

v=0.1 c

v=0.8 c

v=0.95 c

Page 37: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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:

1) 2) 3)

0% 0%0%

1) Longer than your ship2) Shorter than your ship3) Exactly the same as your ship

Page 38: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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:

1) 2) 3)

0% 0%0%

1) Longer than your ship2) Shorter than your ship3) Exactly the same as your ship

2

2

0 1cv

LL

Always <1

Lo > L

In the speeder’s reference frame

In your reference frame

Page 39: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

Comparison:Time Dilation vs. Length Contraction

• to = 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.

2

2

0 1cv

LL

2

2

0 1cv

tt

Lo > L Length seems shorter from “outside”

Dt > DtoTime seems longer

from “outside”

Page 40: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

Relativistic Momentum

Relativistic Momentum2

2

1cv

mvp

Note: for v<<c p=mv

Note: for v=c p=infinity

Relativistic Energy2

2

2

1cv

mcE

Note: for v=0 E = mc2

Objects with mass can’t go faster than c!

Note: for v<<c E = mc2 + ½ mv2

Note: for v=c E = infinity (if m<> 0)

Page 41: Special Relativity Physics 1161: Lecture 35 Sections 29-1 – 29-6.

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


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