Classical Mechanics (Kibble & Berkshire) · Problem 12.19

The calculus of variations and Hamilton's principle — T.W.B. Kibble, F.H. Berkshire

Physics — Mechanics · lagrangian-mechanics-charged-particle-wire-magnetic-field

Problem

A particle of mass mm and charge ee moves in the magnetic field produced by a current II flowing in an infinite straight wire that lies along the zz-axis. The vector potential A\boldsymbol{A} of the induced magnetic field is given by Ar=Aθ=0,Az=−(μ0I2π)ln⁡r,A_r = A_\theta = 0, \qquad A_z = -\left(\frac{\mu_0 I}{2\pi}\right)\ln r, where rr, θ\theta, zz are cylindrical polar coordinates. Find the Lagrangian of the particle. Show that θ\theta and zz are cyclic coordinates and find the corresponding conserved momenta.

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