Relativistic Time Dilation and the Muon Experiment
Pavle I. Premović
Laboratory for Geochemistry,
Cosmochemistry&Astrochemistry,
University of Niš, pavleipremovic@yahoo.com, Niš, Serbia
Abstract
The time dilation of Lorentz-Einstein can be
readily derived from the classical light clock experiment where the clock is positioned
perpendicularly to the direction of its motion. The extent of dilation is given
by the Lorentz factor: 1/√(1-v2/c2) where v is the
relative velocity of the light clock and c is the speed of light.
)
The muon
experiment is apparently consistent with this type of time dilation. Assuming
that the Lorentz-Einstein time dilation is relevant to the light clock
experiment when the clock is aligned along the direction of motion, the Lorentz-Einstein
length contraction is usually then derived. However, if there is no such
contraction we then deal with a time dilation of the non-Lorentz-Einstein type.
The amount of time dilation is now specified by the squared Lorentz factor: 1/(1-v2/c2). It
appears that this type of time dilation is even much more agreeable with the
muon experimental measurements than the Lorentz-Einstein type.
Keywords: Special relativity, Lorentz-Einstein, muon, time
dilation, time contraction.
1. Introduction
Time dilation and length contraction are two
important effects of Special relativity (SR). These two effects depend upon the
second postulate of this theory that the speed of light c is the same in all inertial frames of reference [1, 2]. In
general, the Lorentz-Einstein (LE) time dilation is a prerequisite for the LE
length contraction which only occurs in the direction of motion of the moving
frame [1, 2].
To date,
several indirect LE length contraction experiments were performed [3 – 9] but
no variation in length was measured. Sherwin [10] has reported only one direct experiment and concluded that
it was contradictory to the LE length contraction. As far as we are aware there
is no critical evaluation and possible revision of his experiment. For many researchers, the LE time dilation is indirectly demonstrated by - muon experiment [1]. Most of the information about this experiment presented in this note is taken from
the classic work by Frisch and Smith [7].
According
to SR, the proper time ΔT0 is a time interval of an event
measured by an observer in an inertial frame stationary relative to the event. Moreover, the time interval of the same
event has a longer duration ΔT, called the improper time, as measured by
an observer in an inertial frame moving with a relative speed v to the same
event.
The proper
length in SR is the length of an object in its rest frame. The improper length
is the object's length in any other frame where moving with a
relative speed v.
Many physics textbooks that deal with the concepts of LE time dilation and
length contraction depict using a device known as a light clock [1, 2]. In this
note, we will especially focus our attention on the time dilation and length
contraction when the light clock is positioned along the direction of motion. Of course, you may find all the following
derivations in many elementary physics texts.
2. Discusion and Conclusions
The light clock consists of two plane-parallel mirrors M1 and M2 facing each other at a
distance d apart as in
Fig. 1a. I will here consider only the time intervals while a photon moves
between mirror M1 and mirror M2. The lower mirror M1
has a light source at the center that emits a photon (or a light signal) at 90
degrees in the direction of mirror M2. It is usually assumed
that the photon reaching mirror M2 is back-reflected to mirror M1. Taking into account this assumption, for the light clock
at rest the proper time interval is ΔT0
= 2d/c. However, we must stress here that any photon detection at the
mirror M2 would involve its annihilation.
a
Fig. 1. Measurements and analyses made in different frames. The light clock is positioned
perpendicular to the x-axis. (a): No relative motion. (b): light clock
moving at speed v.
Now allow the same light clock to be moving
with a certain relative speed v horizontally in the direction of the
positive x-axis. An observer in the rest frame who is watching this clock could
design the following diagram, Fig. 1b. A photon will now
travel the larger distance L and thus
it will take a longer (improper) time
ΔT =
2L/c
According to the LE transformation,
ΔT0 and ΔT are
related by the time dilation expression
ΔT =
ΔT0 /√(1-v2/c2)
where 1/√(1-v2/c2) is the Lorentz or time dilation factor.
Let us now
perform the experiments using the same light clock as in Fig 1a but now aligned
along the x-axis, as shown in Fig. 2a. If this clock is resting the time
interval is
ΔT0 = 2d/c.
Fig. 2. Measurements and analysis for the light clock positioned along the
x-axis. (a): No relative motion; (b) and (c): the light-clock moving at
speed v.Allow now this clock to move in the direction of the
positive x-axis with the speed v, Fig.
2 reach the mirror M2 the photon will travel the distance
cΔT+ = D
+ vΔT+
in the time interval
ΔT+ =
D/(c – v)
where D is the length of the light clock measured by a
stationary observer.
For the “back-reflected” photon (Fig. 2c) the time
interval
ΔT- =
D/(c + v)
The total time needed for photon to
complete cycle
ΔT = ΔT+ + ΔT- = 2cD/(c2 - v2)
Factoring out c2 in
the denominator
ΔT = 2D/c(1 - v2/c2)
To acquire a relationship between D
and d one then invokes the LE time dilation
ΔT = ΔT0 /√1-v2/c2 and then write
2D/c(1 - v2/c2) = 2d/c√(1 - v2/c2)
After simplification, we get the LE length
contraction
D = d√(1
- v2/c2)
In this derivation, we hypothesize a priori
that the length of the moving light clock is (of course, relativistically)
different than the proper length: d ≠ D
and the time of this clock is “dilated” relative to the proper time ΔT0 according to the LE
transformation: ΔT = ΔT0 /√(1-v2/c2). However, there is no
experimental evidence corroborating this hypothesis.
Let
us assume first that there is no relativistic
length contraction i. e., D = d then
ΔT =
ΔT0/(1 - v2/c2)
Thus, there is also time dilation but with the squared
Lorentz factor 1/(1 - v2/c2) instead 1/√(1
- v2/c2)
predicted by LE (hereinafter: the non-LE time dilation). It remains to find out
whether the non-LE time dilation agrees with the experiments.
The most convincing
experimental evidence for the time dilation in the direction of the motion
comes from the cosmic muon experiments. Muons are created in the upper Earth’s
atmosphere are secondary products of interactions between primary cosmic rays
and the nuclei of atmospheric molecules. Muons travel at relativistic speeds
and are unstable particles with a mean lifetime at rest T0 ~ 2.2 µs.
At relativistic speeds, the muons experience time dilation. This dilation allows them to reach the Earth’s
surface before they decay. To measure time dilation, the mean lifetime of muons
at rest is compared with the apparent increase in the lifetime of muons in
motion using the measurements of their speeds (v/c) and the changes of muon flux with altitude.
The original
muon experiment was first done by Rossi & Hall [6] in 1941 who measured
muon fluxes at the top of Mt Washington (New England, USA) about 2 km high, and
at the base of the mountain. Their experimental results were consistent with
the relativistic time dilation. The experiment has since been repeated by several
other researchers
.
Let us assume
that the muons are moving vertically down from the height of 10 km at the mean
speed of 0.98c (= 0.98 × 299,792 km s-1 = 293,796 km s-1).
Ignoring relativistic effects, they would travel t ~ 34 µs before reaching
ground level. The fraction of the muons reaching the ground level is given by
P = 2-t/T0 = 2-34/2.2
= 2.2 × 10-3 %
Thus, almost no muons could be expected to reach ground
level.
In light
of the above, the muons moving at a relativistic speed could have a mean
lifetime either of TL = T0 × 1/√(1 - v2/c2)(LE time dilation) or TnL= T0 × 1/(1 - v2/c2) (the non-LE time dilation). Thus, at the mean speed of 0.98c, the mean lifetime of the muons T
could be TL ~ 11 µs or TnL ~ 55 µs. The fraction capable of reaching ground level turns
now into
P = 2-t/T
For the lifetime of TL ~ 11 µs and
TnL ~ 55 µs this fraction would be about 12 % and 65 %, respectively.
Hence, a much larger fraction of the muons (generated in the upper atmosphere) would
be capable of reaching ground level in the non-LE case than in the LE. Besides,
this much higher prediction is even more consistent with experimental
measurements. The question is now how to decide which of these two-time
dilations is right.
Let us assume now that there is no time dilation for the moving light
clock oriented along the direction of motion (i.e., ΔT = ΔT0).
Then it is easy to show that D =
d(1 - v2/c2).
Thus, there is a length contraction by the non-Lorentz factor.
In
conclusion, from the experiment of moving light clock oriented perpendicular to
the direction of motion the demonstration of LE time dilation is simple However, there is no way to illustrate the coexisting LE length
contraction. On the other hand, there is no way to
demonstrate the LE time dilation or length contraction in the case of a moving
light clock positioned along the direction of motion without assuming a priori the
length change according to the LE transformation. However, for this assumption,
there is no experimental evidence.
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