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Time dilation, according to Albert Einstein's
special theory of relativity, is the
slowing-down of the passage of time as experienced by people or objects moving in relation to an observer. Gravitational
time dilation is the slowing down of the passage of time anyplace in the gravitational field.
Velocity time dilation
When one accelerates towards the speed of light, time slows down with respect to the rest of the Universe. That is, a
stationary observer would see the travelling objects slowing down their activity (while still travelling fast). For them, time
passes slower. The effect is of course symmetrical: an observer fixed on the "moving" object sees the "stationary observer"
slowing down.
It is important to note that this effect is extremely small at ordinary speeds, and can be safely ignored for all ordinary
situations. It is only when an object approaches speeds on the order of 30,000 km/s (still 1/10 of the speed of light), that it becomes important.
The formula for determining time dilation factor is:
-
Where T0 is the passage of time measured by a stationary observer and T1 is this passage of time
measured by an observer travelling at velocity v.
| %c |
Length contraction |
Relativistic Mass |
Time dilation |
| 0 |
1.000 |
1.000 |
1.000 |
| 10 |
0.995 |
1.005 |
0.995 |
| 50 |
0.867 |
1.155 |
0.867 |
| 90 |
0.436 |
2.294 |
0.436 |
| 99 |
0.141 |
7.089 |
0.141 |
| 99.9 |
0.045 |
22.366 |
0.045 |
Taken to the extreme, an observer travelling at the speed of light (which, according to special relativity, is impossible for
any object with a non-zero rest mass) would be all but frozen with respect to the
outside world. Massless particles (which are forced by relativity to travel at the speed of light) include photons and gluons. Recently it was determined that neutrinos have a mass, unlike previously thought.
Gravitational time dilation
Gravitational time dilation is a verified effect of general
relativity, and has been experimentally measured using atomic clocks on
airplanes. The clocks that traveled aboard the airplanes were slightly fast with respect to clocks on the ground. The effect is
significant enough that the Global Positioning
System needs to correct for its effect on clocks aboard artificial
satellites, providing a further experimental confirmation of the effect.
An extreme example of gravitational time dilation occurs near a black hole.
A clock falling towards the event horizon would appear (to observers far
away) to slow down to a halt as it approached the horizon. A small and sturdy enough clock could conceivably cross the horizon
without suffering adverse effects at the horizon, but to far away observers it would "freeze" and be flattened out on
the horizon.
Time dilation around a black hole may be described using the following
equation:
Where t0 is time for the object undergoing dilation, tf is time for an observer outside the system, Ch is the circumference of the event horizon, and C0 is the circumference of the object's
orbit about the black hole.
The following chart details the effects of time dilation caused by a black
hole (with a circumference of 10,000 km) for an entity orbiting that black hole, relative to an outside observer. For each
day that passes for the stalwary black hole orbiters, we can determine the amount of time that would pass for an outside
observer.
| Circumference of orbit |
Time experienced by outside
observer per orbiter day |
| 20,000 km |
1.41 days |
| 15,000 km |
1.73 days |
| 12,000 km |
2.44 days |
| 11,000 km |
3.32 days |
| 10,500 km |
4.50 days |
| 10,250 km |
6.40 days |
| 10,050 km |
14.18 days |
| 10,025 km |
20.02 days |
| 10,005 km |
44.73 days |
| 10,000.75 km |
115.47 days |
| 10,000.50 km |
141.42 days |
| 10,000.25 km |
200.00 days |
| 10,000.125 km |
282.84 days |
| 10,000.050 km |
447.21 days |
| 10,000.001 km |
3162.28 days |
In other words, when our orbiter's orbital circumference is merely one meter longer than the circumference of the black hole's
event horizon, about eight years and nine months will pass for the outside observer per orbiter day. If the observer could
somehow watch the action going on inside the orbiter, she would perceive everything as occurring at a staggeringly slow pace,
while the orbiter crew would feel time passing normally. If the crew could watch the life of the outside observer, it would
appear to be passing by at a very fast pace, while the observer would feel time passing normally.
Time dilation and space flight
Time dilation could make it possible to travel "into the future": if we could accelerate a starship enough, one year aboard
the ship might correspond to ten years outside. Indeed, a constant 1g acceleration would permit humans to circumnavigate the
known Universe (with a radius of some 15 billion light years) in under a
subjective lifetime. A more likely use of this effect would be to enable humans to travel to nearby stars without spending their
entire lives aboard the ship. However, any such use of this effect would require an entirely new method of propulsion. A relativistically accelerated object also gains mass, so further
acceleration would require increased amounts of fuel. A further problem with relativistic travel is that the interstellar medium
would turn into a stream of cosmic rays that would destroy the ship unless stark radiation protection measures were taken.
See also
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