A particular type of fundamental particle decays by transforming into an electron e− and a positron e+. Suppose the decaying particle is at rest in a uniform magnetic field of magnitude 3.53 mT and the e− and e+ move away from the decay point in paths lying in a plane perpendicular to images. How long after decay do the e− and e+ collide ?
weird thing is this looks velocity / energy independent they'll both start moving opposite ways round the same circle and all things being even, ie same energy and velocity, they should meet after half a rotation from \(m \omega ^2 r = qvB = q \omega r B\) we have \(\omega = \dfrac{qB}{m} = \dfrac{2 \pi}{T}\) seems to make some sense, but i'd tag michele if it really matters
You have found the cyclotron frequency. In the first cyclotron it worked because the period of revolution was independent of the energy/velocity.
\[\omega = \dfrac{qB}{m} = \dfrac{2 \pi}{T} \implies T = \dfrac{2\pi m}{qB}\]
you want a half period
\[T = \dfrac{2\pi*9.1*10^{-31}}{1.6*10^{-19}*3.53*10^{-3}} \approx 10nS \] http://www.wolframalpha.com/input/?i=%5Cdfrac%7B2%5Cpi*9.1*10%5E%7B-31%7D%7D%7B1.6*10%5E%7B-19%7D*3.53*10%5E%7B-3%7D%7D+
10/2 = 5nS
matches perfectly w/ the textbook answer ! xD
Yes @Farcher we may assume the speeds are much less than the speed of light, so that the period/frequency are independent of velocity/energy :)
Thanks @IrishBoy123
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