On 6/10/2025 8:14 PM, Alan Grayson
wrote:
The
claim is that the muon's half life is increased from its measured
value in the lab frame, to an extended value when observed by a
stationary observer seeing the muon in motion. But how is the lab
frame different from the rest frame in which the muon is is
observed as moving? They seem like the same frame. AG
--
You've confused yourself by not mentioning it's motion in the lab
frame, which is implicitly zero. So it's comparing the half-life in
the muon's frame with the muon's half-life as it travels at near
light speed.
David H. Frisch and Smith (1963) measured approximately 563 muons
per hour in six runs on Mount Washington. By measuring their kinetic
energy, mean muon velocities between 0.995 c and 0.9954 c were
determined. The target was located in Cambridge, Massachusetts with
a difference in height of 1907 m, which should be traversed by the
muons in about 6.4 µs. Assuming a mean lifetime of 2.2 µs, only 27
muons would reach this location if there were no time dilation.
However, approximately 412 muons per hour arrived in Cambridge,
resulting in a time dilation factor of 8.8±0.8.
Frisch and Smith showed that this is in agreement with the
predictions of special relativity: The time dilation factor for
muons on Mount Washington traveling at 0.995 c to 0.9954 c is
approximately 10.2. Their kinetic energy and thus their velocity was
diminished until they reached Cambridge to 0.9881 c and 0.9897 c due
to the interaction with the atmosphere, reducing the dilation factor
to 6.8. So between the start (≈ 10.2) and the target (≈ 6.8) an
average time dilation factor of 8.4±2 was determined by them, in
agreement with the measured result within the margin of errors (see
the above formulas and the image for computing the decay curves).
Brent