Problems in the Schwarzschild Geometry

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Problems in the Schwarzschild geometry April 4, 2015 Start work on the problems below. See the notes on Schwarzschild geodesics to get started. Help is available. Summary of geodesics: We have, for timelike curves: ! dt 1 − 2M = u0 r0 dτ 0 2M 1 − r d' L = dτ r2 r dr 2M L2 2ML2 = 2E + − + dτ r r2 r3 where 2 d' L = r0 dτ 0 " 2 # 1 2M 02 E = − 1 − 1 − u0 2 r0 Problems: dr 1. Find the form of dτ for spacelike and null geodesics. 2. Find the proper time required for a particle to fall from radius r0 > 2M to r = 2M. Evaluate the time numerically for a solar mass black hole, and a galactic black hole with mass 107 times the mass of the sun. 3. Find the proper time required for a particle to fall from radius r0 = 2M to r = 0. Evaluate for solar mass and 107 solar mass black holes. Find predictions for the three classical tests of general relativity. For all three problems, 2M assume r 1. dr 1. Perihelion advance of Mercury. From the orbital equation derived by integrating d' (given in the Notes), find the angle between adjacent minima of r ('). The amount by which this exceeds 2π is the perihelion advance. 1 2. Gravitational red shift. Use your expression for null geodesics, restricted to outward radial motion !0 (L = 0) to find the fractional change in frequency ! (or wavelength) of the light. Remember that the α E ! momentum 4-vector, p = c ; p = ~ c ; k is tangent to the null curve. 3. Deflection of light passing the sun. Again consider a null geodesic but now L 6= 0. Instead, L follows from the point of closest approach, L = r0c where r0 is the impact parameter. The orbit is symmetric around this point, so the integral for r will run from 1 to r0 and back out again. Write the solution as ' = 2 1 F (r) dr where F (r) is what you get from the null geodesic equation. The r0 deviation from a straight´ line is ∆' = 2 1 F (r) dr − π. r0 ´ 2.

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