TIME DILATION

Time is not a physical
constant. Motion and gravity effect time by dilating
(slowing) it or by expanding its duration. In 1905 Albert Einstein
described the effect of motion on time in his special theory of relativity. In
1916 he described the effect of gravity on time in his general theory of
relativity.

Time dilation effects
due to motion were experimentally observed in the early 1970s. Researchers
placed atomic clocks on commercial airliners and observed the expected changes
in time as measured by those clocks relative to similar clocks on the ground.
In particular, when the planes traveled east, in the
direction of Earth’s rotation, the clocks on the airliners were 59 nanoseconds
(59 billionths of a second) slow relative to the atomic clocks on the ground.
When the airplanes traveled west, the clocks were 273
nanoseconds fast. This discrepancy is caused by the rotation of Earth, which
causes an additional time dilation. If the effect of Earth's rotation is
removed, the time dilation produced by the motion of the airliners confirms
Einstein's theory of how time changes with motion, as the dilation is in
agreement with predictions made by the theory.

Time dilation effects
due to gravity have been experimentally verified in many ways. For example,
time on the Sun's surface runs about two parts in a million slower than on
Earth because of the Sun's much higher gravity. In 1968 American physicist
Irwin Shapiro confirmed this effect when he showed that radar signals (see
Radar Astronomy) and their reflections from planets are delayed when the Sun is
near the path of the signals.

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time dilation

also called Time
Dilatation, in the theory of special relativity, the “slowing down” of a clock
as determined by an observer who is in relative motion with respect to that
clock. In special relativity, an observer in inertial (i.e., nonaccelerating) motion has a well-defined means of
determining what events occur simultaneously with a given event. A second
inertial observer, who is in relative motion with respect to the first,
however, will disagree with him regarding which events are simultaneous with
that given event. (Neither observer is wrong in his determination; rather,
their disagreement merely reflects the fact that simultaneity is an
observer-dependent notion in special relativity.) A notion of simultaneity is
required in order to make a comparison of the rates of clocks carried by the
two observers. If the first observer's notion of simultaneity is used, it is
found that the second observer's clock runs slower than his by a factor of Ö(1
- v2/c2), where v is the relative velocity of the observers and c equals
300,000 km (186,000 miles) per second—i.e., the speed of light. Similarly,
using the second observer's notion of simultaneity, it is found that the first
observer's clock runs slower bythe same factor. Thus
each inertial observer determines that all clocks in motion relative to him run
slower than his own clock.

A closely related
phenomenon predicted by special relativity is the so-called clock paradox, or
twin paradox. Suppose an observer carrying a clock departs on a rocket ship
from an inertial observer at a certain time and then rejoins him at a later
time. In accordance with the time-dilation effect, the elapsed time on the
clock of the noninertial observer will be smaller
than that of the inertial observer—i.e., the noninertial
observer will have aged less than the inertial observer when they rejoin.

The time-dilation
effect predicted by special relativity has been accurately confirmed by
observations of the increased lifetime of unstable elementary particles traveling at nearly the speed of light. The clock-paradox
effect also has been substantiated by experiments comparing the elapsed time of
an atomic clock on Earth with that of an atomic clock flown in an airplane. The
latter experiments, furthermore, have confirmed a gravitational contribution to
time dilation, as predicted by the theory of general relativity.