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Length Contraction and Time Dilation

Length Contraction

Material bodies contract when they are moving and this shortening is only in the direction of the motion. If the length of the body is L0, when it is at rest i.e. u = 0, then when it moves with the speed u along its length, then new length L is given by L  = L0 (1 – u2/c2)1/2.

To understand this, consider a spaceship. Suppose, initially the spaceship is at rest and for an observer outside the spaceship, the length of the spaceship is L0 = 50 meters. For the traveller inside the spaceship, the length of the spaceship as seen from inside is say, L01 = 49.8 meters which is less than L0 due to some thickness of the front and the rear parts of the spaceship.

Now, suppose the spaceship is moving with the velocity u along the direction of its length. Suppose the observer, outside the spaceship and at rest, has some divine vision so that he can see the spaceship, even if it is many light years away from him. Suppose, through his divine vision, he can also see inside the spaceship, even when it it is far away from him. For this observer, who is outside the spaceship, the length of the spaceship, which is now moving with the velovity u will appear to be L = L0(1 – u2/c2)1/2. Thus, if the spaceship is moving with the velocity equal to half the velocity of light i.e. u = c/2, then to that observer, the length of the spaceship will appear to be equal to L, where L = L0 (1 – u2/c2)1/2

or L = L0 (1 – 1/4)1/2   (u = c/2 implies u/c = 1/2)

or L0 (3/4)1/2                                                                                                                       

or .866l0

or .866 × 50 = 43.3 meters

Thus, to an observer outside the spaceship and at rest, the length of the moving spaceship, seems to be less than when the spaceship was at rest. For the traveller inside the spaceship, the length of the spaceship as seen from inside will still be L01 = 49.8 meters that is traveller does not feel any difference in the length of the spaceship.

Suppose, the spaceship is moving with the velocity nearly equal to that of light i.e. u = .99c for example. Then, to the observer outside the ship and at rest, the length of the spaceship will appear to be equal to L where L = L0 (1 – u2/c2)1/2

or L = L0 (1 – .992)1/2   (u = .99c implies u/c = .99)

or L = L0 (1 – .9801)1/2  

or L = L0 (.0199)1/2                                                                                                        

or L = 0.141L0

or 0.141 × 50 = 7.05 meters

For the traveller inside the spaceship, the length of the spaceship as seen from inside will still be L01 = 49.8 meters.

Suppose, the spaceship is moving with the velocity u = .9999c. Then, to the observer outside the spaceship and at rest, the length of the spaceship will appear to be equal to L, where L = L0 (1 – u2/c2)1/2

or L = L0 (1 – .99992)1/2   (u = .99c implies u/c = .99)                  

or L =.0141L0

or .0141 × 50 = .705 meters or 70.5 centimeters.

For the traveller inside the spaceship, the length of the spaceship as seen from inside will still be L01 = 49.8 meters.

If spaceship were travelling with the velocity of light i.e u = c, then, to the observer outside the ship and at rest, the length of the spaceship will appear to be equal to L, where L = L0 (1 – u2/c2)1/2

or L = L0 (1 – 1)1/2   (u = c implies u/c = 1)

or L = 0.

For the traveller inside the spaceship, the length of the spaceship as seen from inside will still be L01 = 49.8 meters.

Note that, as per the theory of relativity it is impossible for a body to move with the velocity of light. Thus, the length of the spaceship can never appear to be zero to an outside observer.

Time Dilation

If Δt time interval is passed in a clock moving with the velocity u, then in the same type of clock, which is at rest, Δt / (1 – u2/c2)1/2 time interval will have passed.

Suppose, an observer outside the spaceship has a digital stopwatch, which is reset so that it shows the time as 00:00:00:000 that is 0 hour, 0 minute, 0.00 second. Suppose, the traveller inside the spaceship has the same type of digital stopwatch, which is also reset.

Now suppose, the spaceship is moving with the velocity u and at some time, he presses the start button of his stopwatch. The observer outside the spaceship and at rest, who is observing the traveller inside the spaceship through his divine vision, presses the start button of his stopwatch at the same time, so that both the stopwatch start simultaneously.

Now suppose, some time later, the observer at rest, sees the time elapsed in the stopwatch of the traveller through his divine vision and suppose, he finds that the stopwatch of the traveller is showing 00:00:14:000 i.e. 0 hour, 0 minute 14.000 seconds have elapsed in his stopwatch and at that very time, he stops his own stopwatch and then sees the time elapsed in his stopwatch, then he will find that more than 14 seconds have passed in his stopwatch.

If spaceship were moving with the velocity u = c/2 and if 14 seconds (Δttraveller in spaceship  = 14) seconds had passed in the stopwatch of the traveller inside the spaceship (i.e. The stopwatch of the traveller was showing 00:00:14:000), then in the stopwatch of the observer, time elapsed will be

Δtobserver at rest = Δttraveller in spaceship  / (1 – u2/c2)1/2

Or  Δtobserver at rest  = 14 seconds / (1 – 1/4)1/2       (u = c/2 implies u/c = 1/2 or u2/c2 = 1/4)

Or  Δtobserver at rest  = 16.156 seconds i.e. stopwatch of the observer will show 00:00:16:156 

 

If spaceship were moving with the velocity u = .99c and if 14 seconds (Δttraveller in spaceship  = 14) seconds had passed in the stopwatch of the traveller inside the spaceship, then in the stopwatch of the observer, time elapsed will be

Δtobserver at rest = Δttraveller in spaceship  / (1 – u2/c2)1/2

Or  Δtobserver at rest  = 14 seconds / (1 – .992)1/2       (u = .99c implies u/c = .99)

Or  Δtobserver at rest  = 99.232 seconds i.e. stopwatch of the observer will show 00:01:39:232  (1 min, 39.232 sec)

 

If spaceship were moving with the velocity u = .9999c

Δtobserver at rest  = 14 seconds / (1 – .99992)1/2       (u = .9999c implies u/c = .9999)

Or  Δtobserver at rest  = 989.968 seconds i.e. stopwatch of the observer will show 00:16:29:968  (16 min, 29.968 sec)

Thus, time itself will appear to be slower in a moving spaceship. In other words moving clock ticks slower.

If the observer outside the spaceship and at rest sees that the traveller inside the spaceship is having dinner, then all the motions (eg, taking food in the spoon, thrusting the spoon in the mouth, pulling the spoon out of the mouth, chewing the food, drinking a glass of water) of the traveller appear to be slower than the normal, while to the traveller inside the spaceship, everything moves at the normal rate, that is not only does the length shorten but also the clock slows down. That is when the clock inside the spaceship records 1 second elapsed, as seen by the traveller inside the spaceship, the same type of clock near the observer outside the spaceship and at rest shows 1 / (1 – u2/c2)1/2 seconds, which is more than 1 second.

Suppose, in addition to observer at rest, the traveller also has the divine vision and the traveller is now watching the person who was observer and who is outside the spaceship and at rest. For the traveller, time is moving with the same normal speed in both the cases i.e. when the spaceship is moving along at a uniform speed as well as when the spaceship is at rest.

Now, if the person who was the observer, is having dinner, then to the eyes of the traveller, all the motions (eg, taking food in the spoon, thrusting the spoon in the mouth, pulling the spoon out of the mouth, chewing the food, drinking a glass of water) of that person appear to be faster than the normal, while to the person (who was observer and is now being observed by the traveller inside the spaceship), everything moves at the normal rate. Thus, for the traveller, velocity of time outside the spaceship appear to be increased by the factor 1 / (1 – u2/c2)1/2.  If 14 seconds passed inside spaceship, which is moving with the speed u = c/2,  14/ (1 – u2/c2)1/2 or 16.156 seconds will have passed outside the spaceship.

To the observer outside the spaceship and at rest, the length of the spaceship appears to be contracted.

Similarly,  to the traveller inside the spaceship, the distance between the spaceship and the observer (who is now being observerd by the traveller) appear to be contracted. This is explained in the next example.

 
Length Contraction and Time Dilation

Suppose the spaceship is 100 light seconds away from the observer and is moving with velocity u = .8c towards the observer.

(one light second is the distance travelled by light in one second i.e. 1 light second = 299792452 meter/sec × 1sec = 299792452 meters).

 Suppose, when the spaceship is 100 light seconds away , the traveller inside the spaceship resets & starts his stopwatch and at the same time, the observer at rest does the same. 

When the spaceship reaches to the observer, time elapsed in the stopwatch of the observer will be 'distance / velocity' = 100 light seconds / 0.8c = (100 × 299792452 meters) / (0.8 × 299792452 meters/second) =125 seconds. Thus, the stopwatch of the observer will show 00:02:05:00 i.e. 2 min, 5 sec.

Now from Δtobserver at rest = Δttraveller in spaceship  / (1 – u2/c2)1/2

Δttraveller in spaceship  = Δtobserver at rest × / (1 – u2/c2)1/2

The spaceship is moving with the velocity u = 0.8c. Thus, (1 – u2/c2)1/2 = (1 – 0.82)1/2 = 0.6

Thus, Δttraveller in spaceship  = Δtobserver at rest × 0.6 = 125 × 0.6  = 75 seconds that is, for the traveller, he completed the journey ( which was of 100 light seconds for the observer outside the spaceship and at rest), when in his stopwatch 75 seconds had passed that is, for the traveller, in actual, 75 seconds had passed inside the spaceship during his journey and during these 75 seconds, moving with the velocity u = 0.8c, the spaceship will travel 0.8c × 75 sec = 60 light sec (or 60 × 299792452 meters).

Thus, the traveller inside the spaceship will say, the journey was of 60 light seconds (which he completed in 75 seconds moving with the velocity u = .8c). But the observer at rest will say, the journey was of 100 light seconds (which the traveller completed in 125 seconds moving with the velocity u = .8c).

This contradiction disappears, if we consider the length contraction that is as the spaceship was moving towards the observer, the distance between the spaceship and the observer, as seen by the traveller will be L = L0 (1 – u2/c2)1/2 = 100 light second× (1 – 0.82)1/2 = 100 light second× 0.6 = 60 light seconds.

Thus, for the observer at rest, this journey was of 100 light seconds, which the traveller completed in 125 seconds moving with the velocity u = 0.8c.

For the traveller, this journey was of 100 × (1 – u2/c2)1/2 light seconds, which the traveller completed in 125 × (1 – u2/c2)1/2 seconds moving with the velocity u = 0.8c. 

u = 0.8c implies (1 – u2/c2)1/2 = 0.6. Thus, for the traveller, this journey was of 100 × 0.6 = 60 light seconds, which the traveller completed in 125 × .6 = 75 seconds while moving with the velocity u = 0.8c.

 


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SENTENCE PRACTICE - 1

SENTENCE PRACTICE - 2

SENTENCE PRACTICE - 3

Useful Facts About Daily Life

RAQ

Length Contraction
and
Time Dilation

About The Mysterious....

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