Classical Mechanics (Kibble & Berkshire) · Problem 4.33

Linear oscillations — T.W.B. Kibble, F.H. Berkshire

Physics — Mechanics · circular-motion-magnetron

Problem

The magnetron An electron of mass mm and charge −e-e is moving under the combined influence of a uniform electric field E0jE_0\boldsymbol{j} and a uniform magnetic field B0kB_0\boldsymbol{k}. Initially the electron is at the origin and is moving with velocity uiu\boldsymbol{i}. Show that the trajectory of the electron is given by x=a(Ωt)+bsin⁡Ωt,y=b(1−cos⁡Ωt),z=0,x = a(\Omega t) + b\sin\Omega t, \quad y = b(1-\cos\Omega t), \quad z = 0, where Ω=eB0/m\Omega = eB_0/m, a=E0/ΩB0a = E_0/\Omega B_0 and b=(uB0−E0)/ΩB0b = (uB_0 - E_0)/\Omega B_0. Use computer assistance to plot typical paths of the electron for the cases a<ba < b, a=ba = b and a>ba > b. [The general path is called a trochoid, which becomes a cycloid in the special case a=ba = b. Cycloidal motion of electrons is used in the magnetron vacuum tube, which generates the microwaves in a microwave oven.]

Related theory

Browse the problem library