GR problem set 02
We dene covariant derivative of a vector as:
∇αuµ≡ uµ;α = uµ,α+ Γµαβuαuβ, where uµ,α ≡ ∂αuµ≡ ∂uµ
∂xα. Covariant derivatives of other tensors is dened using the properties:
∇α(uµvµ) = ∂α(uµvµ) (for scalar φ,α ≡ φ;α)
∇α(uµvν) = vν∇αuµ+ uµ∇αvν (Leibniz' rule)
16. We want ∇αuµ to be a tensor (with a proper tensor transformation rule). Then, how should the transformation law for Γµαβ look like?
17. Show (with explicit calculation) that there is one and only one connection (called metric connection) that is symmetric (Γγαβ = Γγβα) and fullls ∇αgµν = 0 condition.
∇αgµν = ∂αgµν− Γραµgρν− Γρναgρµ.
18. Find the metric connection components for the Euclidean metric ds2 = dx2 + dy2 in polar coordinates.
19. Show that (a)
Γααβ = 1 2g
∂g
∂xβ , where g = | det(gαβ)|.
(b) then using (a) show
∇αvα = 1
√g∂α(√
gvα), ∇α∇αΦ = 1
√g∂α√ggαβ∂βΦ for any vector and scalar eld, vα and Φ respectively.
20. Show that for any curve with a tangent vector vα such that vα∇αvβ = cvβ, where c is an arbi- trary function on the curve, one can nd a parametrization such that in this parametrization vα∇αvβ = 0 holds (ane parametrization). Show that two dierent ane parametrizations are connected with a linear transformation.
(∇µ∇ν − ∇ν∇µ)uα is linear in u and does not contain any derivatives of u (please check). Thus we can write:
(∇µ∇ν− ∇ν∇µ)uα = Rαβµνuβ, This denes the Riemann tensor Rαβµν.
We also dene: Rβν = Rαβαν (Ricci tensor) and R = gβνRβν (Ricci scalar).
21. Show the following symmetry properties for the Riemann tensor:
(a) Rαβµν = Rµναβ = −Rαβνµ = −Rβαµν , (b) Rαβµν+ Rανβµ+ Rαµνβ = 0 ,
(c) Rαβµν;λ+ Rαβλµ;ν+ Rαβνλ;µ = 0 (Bianchi identities), (d) (Rαβ − 12gαβR);β = 0 (contracted Bianchi identities).
Hint: (a)-(c) can be easily checked in a locally Lorentzian frame (cf problem 15), then (d) follows from (c).
22. Show that, in n-dimensional space the Riemann tensor has (in general) n2(n2− 1)/12 inde- pendent components.
A. Rostworowski http://th.if.uj.edu.pl/ arostwor/