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2 Show that Γ

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(1)

1 Calculate the Christoel symbols for the Euclidean metric ds

2

= dx

2

+ dy

2

in polar coordinates.

2 Show that Γ

ααβ

= 1 2g

∂g

∂x

β

, where g = det(g

αβ

) . Using that show that for a vector eld v

α

and a scalar eld Φ we have

α

v

α

= 1

p|g| ∂

α

(p|g|v

α

), ∇

α

α

Φ = 1

p|g| ∂

α

hp

|g| g

αβ

β

Φ i

3 Show that the anely parametrized geodesic equation is the Euler-Lagrange equation for the action

S[x

µ

(s)] = Z

g

αβ

(x) dx

α

ds

dx

β

ds ds .

4 Find all timelike geodesics on the Lorentzian manifold M = {(t, x) ∈ R

+

× R} with the metric ds

2

= t

−2

(−dt

2

+ dx

2

) .

5 Consider the 2-sphere with the metric ds

2

= dθ

2

+ sin

2

θ dφ

2

.

(a) Write down the geodesic equation and show that the lines of constant φ are geodesics but the lines of constant θ are not geodesics unless θ = π/2.

(b) A vector v

α

is parallely transported from a point (θ

0

, φ

0

) to a point (θ

0

, φ

1

) along the

curve (θ

0

, φ

0

+ λ) . Find v

α

(λ) .

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