Covariant derivative of vector fields on the sphere

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The discussion revolves around calculating the covariant derivatives of two vector fields, W_ρ and U^ρ, on a sphere. Participants detail their calculations for D_v W_ρ and D_v U^ρ, using the provided equations and Christoffel symbols. A check is performed to verify the identity involving the derivatives and the product of the vector fields, leading to clarification on the summation over indices. The conversation highlights a misunderstanding regarding the completeness of the expression, which is resolved by recognizing the need for summation over the index ρ. Ultimately, the calculations confirm that the terms cancel appropriately, validating the identity.
Whitehole
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Homework Statement


Given two vector fields ##W_ρ## and ##U^ρ## on the sphere (with ρ = θ, φ), calculate ##D_v W_ρ## and ##D_v U^ρ##. As a small check, show that ##(D_v W_ρ)U^ρ + W_ρ(D_v U^ρ) = ∂_v(W_ρU^ρ)##

Homework Equations


##D_vW_ρ = ∂_vW_ρ - \Gamma_{vρ}^σ W_σ##
##D_vU^ρ = ∂_vU^ρ + \Gamma_{vσ}^ρ U^σ##

##\Gamma_{φφ}^θ = -sinθ~cosθ, ~~~~~\Gamma_{θφ}^φ = \frac{cosθ}{sinθ}##

The Attempt at a Solution


I've calculated all the problem asked as

##D_θW_θ = ∂_θW_θ, ~~~~~~~ D_θW_φ = ∂_θW_φ - \frac{cosθ}{sinθ}W_φ##

##D_φW_θ = ∂_φW_θ - \frac{cosθ}{sinθ}W_φ, ~~~~~~~ D_φW_φ = ∂_φW_φ + sinθ~cosθ~W_θ####D_θU^θ = ∂_θU^θ, ~~~~~~~ D_θU^φ = ∂_θU^φ + \frac{cosθ}{sinθ}U^φ##

##D_φU^θ = ∂_φU^θ - sinθ~cosθ~U^φ, ~~~~~~~ D_φU^φ = ∂_φU^φ + \frac{cosθ}{sinθ}U^θ##

For the check,

##(D_θW_φ)U^φ + W_φ(D_θU^φ) = (∂_θW_φ - \frac{cosθ}{sinθ}W_φ)U^φ + W_φ(∂_θU^φ + \frac{cosθ}{sinθ}U^φ)##

The second and the fourth term obviously cancels so it satisfies the equality.

I'm stuck here,

##(D_φW_θ)U^θ + W_θ(D_φU^θ) = (∂_φW_θ - \frac{cosθ}{sinθ}W_φ)U^θ + W_θ(∂_φU^θ - sinθ~cosθ~U^φ)##

The second and the fourth term do not cancel each other, also U and W doesn't match each others subscript/superscript. What I'm thinking is to transform either U or W so that the subscript/superscript will match but I'm not sure how to do it. Any suggestions?
 
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Whitehole said:
For the check,

##(D_θW_φ)U^φ + W_φ(D_θU^φ) = (∂_θW_φ - \frac{cosθ}{sinθ}W_φ)U^φ + W_φ(∂_θU^φ + \frac{cosθ}{sinθ}U^φ)##
The left hand side is not the complete expression that you want to look at. You need to write out the left side of ##(D_v W_ρ)U^ρ + W_ρ(D_v U^ρ) = ∂_v(W_ρU^ρ)##. Note the summation over the index ##\rho## while the index ##v## is held fixed.
 
TSny said:
The left hand side is not the complete expression that you want to look at. You need to write out the left side of ##(D_v W_ρ)U^ρ + W_ρ(D_v U^ρ) = ∂_v(W_ρU^ρ)##. Note the summation over the index ##\rho## while the index ##v## is held fixed.
What do you mean it is not complete? Do you mean, the right hand side? I forgot that it is a summation on ρ.

##(D_θW_θ)U^θ + (D_θW_φ)U^φ + W_θ(D_θU^θ) + W_φ(D_θU^φ) = ∂_θW_θU^θ + ∂_θW_φU^φ - \frac{cosθ}{sinθ}W_φU^φ + W_θ∂_θU^θ + W_φ∂_θU^φ + \frac{cosθ}{sinθ}W_φU^φ##

It should be like this right? Then for the case where ##D_φ##, I can already see that the terms that I thought will not cancel, should already cancel.
 
That looks good.
 
TSny said:
That looks good.
Thanks for the reminder!
 

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