A particle of rest mass moves at constant speed around a circle of radius in the…

PHYSICS · Multi-part · Fermi University Physics · Relativity & Gravitation · Special relativity: spacetime and kinematics · Relativistic dynamics and fields in flat spacetime

The Geometry of Gravity, Ch Minkowski spacetime and relativistic dynamics, completed

Problem

A particle of rest mass mm moves at constant speed vv around a circle of radius rr in the laboratory frame, with angular speed ω=v/r\omega=v/r, so that its position at laboratory time tt is (x,y)=(rcos⁡ωt, rsin⁡ωt)(x,y)=(r\cos\omega t,\,r\sin\omega t). ((a)) Write uμu^\mu at an arbitrary time tt, and find aμ=duμ/dτa^\mu=du^\mu/d\tau there, in terms of γ\gamma, cc, vv, rr and ωt\omega t. ((b)) Show that uμaμ=0u_\mu a^\mu=0 at every tt, and find the proper acceleration aa, defined by aμaμ=a2a^\mu a_\mu=a^2, in terms of γ\gamma, vv and rr. ((c)) Find the four-force fμf^\mu that keeps the particle on the circle, assuming its rest mass does not change. What does its time component say about the work done on the particle, and how large is the three-force ∣F⃗∣|\vec F| that must act? ((d)) Evaluate aa for v=0.60cv=0.60c and r=1.0 kmr=1.0\ \mathrm{km}, and express it as a multiple of one Earth gravity, 9.81 m s−29.81\ \mathrm{m\,s^{-2}}.

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