An Introduction to Modern Astrophysics · Problem 16.23

General Relativity and Black Holes — Carroll & Ostlie

Physics — Astrophysics · pulsar-magnetosphere-charged-particles

Problem

One way of qualitatively understanding the flow of charged particles into a pulsar's magnetosphere is to imagine a charged particle of mass mm and charge ee (the fundamental unit of charge) at the equator of the neutron star. Assume for convenience that the star's rotation carries the charge perpendicular to the pulsar's magnetic field. The moving charge experiences a magnetic Lorentz force of Fm=evBF_m = evB and a gravitational force, FgF_g. Show that the ratio of these forces is FmFg=2πeBRPmg,\frac{F_m}{F_g} = \frac{2\pi eBR}{Pmg}, where RR is the star's radius and gg is the acceleration due to gravity at the surface. Evaluate this ratio for the case of a proton at the surface of the Crab pulsar, using a magnetic field strength of 10810^8 T.

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