Savchenko Problem 14.4.1

Physics · electromagnetism · modern-physics · relativity

Problem

An electron entering an extended stationary and uniform electric field at the velocity β\betac departs from it after a time τ\tau The electron velocity is directed along the field. How long will an electron stay in the field if, on the contrary, the field hits a stationary electron with the same speed? Solve this problem in two ways, using: a) relativistic deceleration effect of time, b) the Lorentz formula, according to which the mass of a particle moving at a speed of β\betac, m = mi1−β2\frac{m_i}{\sqrt{1-\beta^2}}, where mim_i is the rest mass of the particle. *) If the problem does not require a numerical answer, denote the rest mass of the electron mem_e, the charge e.

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