An Introduction to Modern Astrophysics · Problem 17.20

Close Binary Star Systems — Carroll & Ostlie

Physics — Astrophysics · black-holes-frame-dragging

Problem

(a) The angular rotation rate, Ω\Omega, at which spacetime is dragged around a rotating mass must be proportional to its angular momentum LL. The expression for Ω\Omega must also contain the constants GG and cc, together with the radial coordinate rr. Show on purely dimensional grounds that Ω=constant×GLr3c2,\Omega = \text{constant} \times \frac{GL}{r^3 c^2}, where the constant (which you need not determine) is of order unity. (b) Evaluate this for Earth, assuming that it is a uniformly rotating sphere. Set the leading constant equal to one, and express your answer in arcseconds per year. How much time would it take for a pendulum at the north pole to rotate once relative to the distant stars because of frame dragging? (c) Repeat part (b) for the fastest known pulsar, expressing Ω\Omega in revolutions per second.

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