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Physikalisches Institut Exercise 10

Universit¨ at Bonn 22 June 2011

Theoretische Physik SS 2011

Exercises on General Relativity and Cosmology

Priv. Doz. Dr. S. F¨ orste

–Home Exercises–

Due 29 June 2011

Exercise 10.1: Einstein equation (2 credit s )

(a) In a local region of spacetime, an observer finds that the Ricci scalar is nearly con- stant, R ≈ +1/a

2

. What can you say about the equations of state of the matter sourcing this curvature? If the region of spacetime is filled only with electromagnetic

energy, what is R? (1 credit )

(b) Is it possible to have a solution of the Einstein equations, in which space is empty to the past of some surface of constant time t = 0, but in which there is a nonvanishing

T

µν

to the future of this surface? (1 credit )

Exercise 10.2 Motion in Schwarzchild geometry (18 credit s ) (a) A particle falls radially into a Schwarzschild metric.

(i) As measured by proper time at infinity, what is its inward coordinate velocity

(dr/dt) at a (curvature-) radius r? (3 credit s )

(ii)What is the locally-measured velocity relative to a stationary observer at the same

radius? (2 credit s )

(b) Derive the equations of motion (ie. equations relating t, r and proper-time τ) for a particle falling radially in the Schwarzschild geometry. Consider the three cases:

(i) particle released from rest at r = R (3 credit s )

(ii) particle released from rest at infinity (3 credit s ) (iii) particle projected inward from infinity with velocity v

. (2 credit s ) (c) Show that the trajectory of light rays in the Schwarzschild metric obeys:

d

2

u

2

+ u = 3u

2

where, u = M/r and r is the Schwarzschild radial coordinate. Denote the minimum value of r along the trajectory by b, the impact parameter. In case of (M/b) << 1, what is the deflection of a photon as it passes a spherical gravitating body? Give a formula for the deflection angle to lowest nonvanishing order in (M/b). (5 credit s )

1

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