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RELATIVITY
Einstein published two theories of relativity
In 1905
The Special Theory
For uniform motion 0a =
In 1916
The General Theory
For non-uniform motion 0a ≠ .
2
First we will discuss The Special Theory
At the beginning of the century most believed
light was a wave.
Thus must have something that waves:
Sound has air
Water has water, etc.
3
Physicists proposed that for waves of light
something must wave.
They called it the “ether” for light
This ether then must fill the universe.
The earth moves through the universe so:
How fast are we traveling through the ether?
To answer this we will start with a race
between two boats (that run at exactly the same
speed) in a river.
5
The calculated time for round trip is
// 2 2
2L L Lctc v c v c v
= + =+ − −
The speed for the boat going cross-stream will
have speed both ways
2 2c v−
Therefore
2 2
2cross
Ltv c
=−
Then the ratio of the two times will be
6
/ /2
2
1 11c r o s s
tt v
c
= >
−
Therefore we see that the boat that goes across
and back wins the race even though both boats
travel the same speed relative to the water.
The main point is the time to complete the
race is different for the two boats.
Note:
7
We can measure ratio of times for boats and
calculate the speed of river if we know the
speed of boats.
9
Drawing of actual apparatus
We know the speed of light.
We want the speed of the earth through the
ether.
10
When light arrives at the eye it has traveled two
paths to reach the observer.
There will be interference – either
constructive
or
destructive
The resulting image will be a series of lines.
11
Spectrometer lines
Since the direction of the ether flow is not
known the apparatus must be rotated.
12
First one than the other path will be parallel to
the flow of ether.
Therefore the interference lines should shift.
Michelson and Morley did the experiment very
carefully and did not find a shift.
The conclusion has to be that:
The Ether does not exist
or
the earth travels along with it.
13
Another experiment shows that we are
not moving with it.
Stellar Aberration is that experiment
While the light travels down the telescope the
telescope moves with the earth.
14
The telescope has to be tilted to keep the image
in the center.
If the ether (the substance that waves to cause
the propagation of light) moves with the scope
there would be no need to tilt the it.
Therefore we conclude the ether does not
exist.
Classical Relativity
The transformation equations before Einstein
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'
'
'
'
x x v t
y y
z z
t t
= −
=
=
=
These are the Galilean Equations that allow
observers to compare observations in two
different frames moving relative to each other
with constant velocity.
16
Observer on ground and observer on railroad
car moving in x-direction.
The observer on the ground observes the birds
separated by distance 2 1x x− .
The distances are equal.
17
If an airplane flies over the railroad car
traveling in the x+ direction at a speed xu
measured by the observer on the ground what
will be the speed ( 'xu ) of the airplane measured
by the observer on the railroad car?
We can use the transformation equation for x
'x x vt= −
and the equation for t
't t=
Differentiate and divide to get
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'dx dx dvv t
dt dt dt= − −
' 0x xu u v= − −
if the velocity of the railroad car is constant.
If the observer on the ground measures the
velocity of the airplane as
xu
then the person on the railroad car will measure
'xu
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What if the person on the ground points a
flashlight in the x+ direction? What will be
the speed of light measured by the observer on
the railroad car?
20
We get
'
'
x xu u vgivingc c v
= −
= −
We must keep this result in mind as we discuss
Einstein’s Theory.
21
Einstein’s postulates for the Special Theory of
Relativity:
1. Fundamental laws of physics are identical
for any two observers in uniform relative
motion.
2. The speed of light is independent of the
motion of the light source or observer.
22
These postulates cannot be satisfied using the
Galilean Equations, as we will see.
However Einstein found that the following
equations worked.
2
2
2
' ( )''
' ( )
1
1
x x vty yz z
vxt tc
where
vc
γ
γ
γ
= −==
= −
=
−
23
These are the Lorentz Transformation
Equations.
Now consider the airplane flying over the
railroad car in the x-direction. What is the
speed of the airplane as measured by the
observer on the ground? What is the speed of
the airplane as measured by the observer on the
railroad car? We need to answer these
questions by using the Einstein-Lorenze
Equations.
24
2
2
2
' ( )
' ( )
' ( )
' ( )
''
x x vtand
vxt tc
differentiatedx dx vdtand
vdxdt dtc
dividedx dx vdt
vdxdt dtc
γ
γ
γ
γ
= −
= −
= −
= −
−=
−
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divide by 'dt
2
'
2
''
1
1
xx
x
dx vdx dtdxdt vdt
cor
u vu vuc
−=
−
−=
−
Thus if an object (an airplane) flies over the
railroad car the observer on the ground will
26
measure the speed in the x direction as xu . The
observer on the car will find 'xu .
What about the speed of light when a flashlight
is pointed in the x-direction?
The observer on the ground points a flashlight
in the +x direction. What will be the speed of
light measured by the observer on the car?
'
2( ) /1 1
xc v c v c vu cvc v c v c
c c
− − −= = = =
−− −
27
Both observers, even though they are moving
relative to each other, measure the same value
for the speed of light.
This is in agreement with the Second Postulate.
LENGTH CONTRACTION
Read the section on Length Contraction in the
book. We will do it a little differently.
28
The observer on the moving railroad car has a
rod moving with him. He measures the length
of the rod to be
' '2 1 0x x L− =
Use the Lorentz equations to get
'2 2 2
'1 1 1
( )
( )
x x vt
x x vt
γ
γ
= −
= −
Then putting these in the equation
29
[ ]
0 2 2 1 1
0 2 1 2 1
( ) ( )
( ) ( )
L x vt x vt
L x x v t t
γ γ
γ
= − − −
= − − −
If the observer on the ground measures the far
end and near end of the rod at the same time
1 2t t=
Then
0 2 1( )L x x Lγ γ= − =
or
0LLγ
= and γ > 1
30
So the observer on the ground with the rod
moving past in the x direction measures the rod
to be shorter than what is measured by the
observer at rest relative to the rod and on the
car.
Length Contraction is a prediction of the
Lorentz Equations.
TIME DILATION
Again we will find time dilation a different way
than the book. Then we will analyze the book’s
method.
31
Observer on railroad car moving in x-direction
with firecrackers and another observer on
ground.
There is a firecracker on the top of the pole at
'1x and one on the top of the pole at
'2x . Let’s
say the firecracker on the top of the pole at '1x
explodes and then some time later the one on
32
top of the pole at '2x explodes. We want to
consider the time between the two events.
The time interval between the two events as
measured by the observer on the ground will be
2 1t t t∆ = −
Using the transformation equations we get
'' 2
2 2 2
'' 1
1 1 2
( )
( )
v xt tc
v xt tc
γ
γ
= +
= +
So
33
' '' '2 12 12 2
' ' '2 12
( ) ( )
( ( )
vx vxt t tc c
or
vt t x xc
γ γ
γ
∆ = + − +
⎡ ⎤∆ = ∆ + −⎢ ⎥⎣ ⎦
The time interval is different for the two
observers.
For simplicity consider two firecrackers on the
same post at
' ' '1 2x x x= =
then
34
' ' ' '
2 12 ( )vt t x x tc
γ γ⎡ ⎤∆ = ∆ + − = ∆⎢ ⎥⎣ ⎦
and
1γ >
So the time interval for the observer on the
ground with the events moving relative to him
is longer.
MOVING CLOCKS RUN SLOWLY
If an observer is moving relative to a clock
the interval between ticks will be longer.
This is Time Dilation
36
For the girl on the railroad car, O’ frame, the
light travels up and back to the floor.
The distance traveled is 2d
The time to travel is ∆t’
The speed of light is c
So
' 2dtc
∆ =
37
The observer on the ground sees the light travel
from the floor to the ceiling but during this time
the railroad car moves carrying the mirror with
it at a speed v.
38
The observer on the ground sees the light travel
farther when it goes from floor to ceiling than
the observer on the railroad car.
For the girl distance traveled = d
For the boy distance traveled = 2c t∆
Both observers must measure the speed of light
as c.
Therefore, since the distance traveled is longer
for the boy than for the girl
40
We see that
2 2
2
2 2c t v t d∆ ∆⎛ ⎞ ⎛ ⎞= +⎜ ⎟ ⎜ ⎟
⎝ ⎠ ⎝ ⎠
Solve for t∆
2 2
2 2
4 4c vt d
⎛ ⎞∆ − =⎜ ⎟
⎝ ⎠
or
22
2 2
4dtc v
∆ =−
and
41
2 2 2
2
2 2
1
d dtc v vc
c
∆ = =−
−
Use
' 2dtc
∆ =
to get
'2d c t= ∆
and put in above equation to get
43
Einstein / Lorentz Transformation Equations
1. Satisfy Einstein’s Second Postulate
2. Predict Length contraction
3. Predict Time Dilation
But are these correct?
Must have an experiment to prove!!!
44
Muon “lifetime” Experiment
Muons are particles created high in our
atmosphere.
They rain down continuously at high velocity at
approximately 82.994 10v x= m/s.
If at rest they only exist for approximately 62 10xτ −= seconds.
The experiment is to set up a detector at the top
of a mountain and stop the muons in the
detector and measure how long they exist.
45
Then ask how far down would they have
traveled if they had not been stopped in the
detector.
distance = (speed) x (time they exist) 8 6(2.994 10 / ) (2 10 )d x m s x x s−=
= 600 m.
If the mountain is 2000m tall, at bottom should
find very few if any muons.
46
Move the apparatus to the bottom of the
mountain and measure the number of the same
type muons that reach sea level.
The experiment showed that as many reached
sea level as passed through the atmosphere at
the level of the top of the mountain.
Why?
When moving relative to us the observer they
exist not for τ = 2 x 10-6 s but for
47
6 6
82
8
16 16(2 10 ) 32 102.994 101 ( )
3 10
tt t x s x sx
x
τ γ − −= = = = =
−
Thus distance traveled will be 8 6(2.994 10 / )(32 10 ) 10,000d x m s x s m−= =
well below sea level.
Or viewed from the muon