Dale
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OK, so I will use units where c=1, and the decay law in post 13: n=n_0 e^{-\lambda \tau}. Assuming that the initial number and the decay constant are known then all that remains is to calculate tau for two cases, one being muons in a cyclotron and the other being muons at rest in the lab. We will neglect gravity and, since cyclotrons are circular it will be convenient to use cylindrical coordinates. The flat spacetime metric in cylindrical coordinates is: d\tau^2=dt^2-dr^2-r^2d\theta^2-dz^2 and, as mentioned in post 37, \tau_P=\int_P d\tauuniversal_101 said:But if you think, that comparing the decay of Muons in lab and in cyclotrons does not involve the gamma factor. Please post some calculations for the same.
For the first case, the muons in the cyclotron, we can write their worldline as P=(t,r,\theta,z)=(a T, R, a 2 \pi, 0) where a is the number of "laps" around the cyclotron, R is the radius of the cyclotron, and T is the period for one lap. So we have
\tau_P=\int_P d\tau=\int_0^a \frac{d\tau}{da}da=\int_0^a \sqrt{\frac{dt^2}{da^2}-\frac{dr^2}{da^2}-r^2\frac{d\theta^2}{da^2}-\frac{dz^2}{da^2}} \; da=\int_0^a \sqrt{T^2-0-R^2 4 \pi^2-0} \; da=a\sqrt{T^2-4\pi^2 R^2}
For the second case, the muons at rest in the lab, we can write their worldline as P=(t,r,\theta,z)=(a T, R, 0, 0). So we have
\tau_P=\int_P d\tau=\int_0^a \frac{d\tau}{da}da=\int_0^a \sqrt{\frac{dt^2}{da^2}-\frac{dr^2}{da^2}-r^2\frac{d\theta^2}{da^2}-\frac{dz^2}{da^2}} \; da=\int_0^a \sqrt{T^2-0-R^2 0-0} \; da=aT
So, I have calculated the number of decayed particles for particles at rest in the lab and in a cyclotron without using \gamma = (1-v^2)^{-1/2}.