Is the Gradient of a Contravariant Vector a Covariant Vector?

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The discussion centers on the relationship between contravariant vectors and their gradients in both flat and curved spaces. The expression for the differential of a contravariant vector field, dVμ = (∂Vμ/∂xη)dxη, is analyzed, with the conclusion that the term on the right-hand side is a covariant tensor. It is established that in curved space, the partial derivative ∂νVμ does not behave as a tensor, while the covariant derivative ∇νVμ does represent a tensor of mixed type. The challenge lies in demonstrating that the gradient of a contravariant vector is indeed a covariant vector.

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nigelscott
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I have:

dVμ = (∂Vμ/∂xη)dxη where Vμ is a contravariant vector field

I believe the () term on the RHS is a covariant tensor. Is the dot product of () and dxη a scalar and how do I write this is compact form. I know how this works for scalars but am not clear when tensors are involved.
 
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nigelscott said:
I have:

dVμ = (∂Vμ/∂xη)dxη where Vμ is a contravariant vector field

I believe the () term on the RHS is a covariant tensor. Is the dot product of () and dxη a scalar and how do I write this is compact form. I know how this works for scalars but am not clear when tensors are involved.

You haven't been very specific. What kind of space are you in? Is it flat or curved?

Generically speaking, ##\partial_\nu V^\mu## is not a tensor at all, because in curved space, partial derivatives do not transform nicely under changes of coordinates. Using a covariant derivative,

\nabla_\nu V^\mu
is a tensor of mixed type.

In curved space, "##\mathrm{d} V^\mu##" is not really a sensible thing to do, because it is not covariant under coordinate changes.
 
Flat space. I am trying to show that the gradient of a contravariant vector is a covariant vector. I understand how to show this for a scalar, but not sure how to extend this to vectors/tensors.
 

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