Divergence of mixed II-order tensors

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The divergence of a second-order mixed tensor in curvilinear coordinates is defined by contracting lower indices with upper indices, specifically using \nabla_i N^i_j. The choice of which index to contract affects the physical interpretation of the tensor, as it relates to the conservation of different quantities represented by the tensor. For example, the divergence of the energy-momentum tensor can indicate covariant conservation depending on the context. Understanding the specific meaning of the tensor components is crucial for accurate interpretation. The discussion emphasizes the importance of correctly applying tensor calculus in physical applications.
enzomarino
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Dear friends,
How is the divergence in curvilinear coordinates of a second order mixed tensor defined? I mean, shall I contract the covariant or the contravariant index?? And for both cases which is the physical meaning?

\nabla_i N^i_j or \nabla_j N^i_j?

Thanks a lot,
Enzo
 
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enzomarino said:
Dear friends,
How is the divergence in curvilinear coordinates of a second order mixed tensor defined? I mean, shall I contract the covariant or the contravariant index?? And for both cases which is the physical meaning?

\nabla_i N^i_j or \nabla_j N^i_j?

Thanks a lot,
Enzo


You should always contract lower indices with upper indices in the first place. I think you're confused because the energy momentum tensor T is symmetric, so it doesn't mind with which index you contract.

The physical meaning of the divergence depends on what the tensor T represents; it depends on what the T^{\alpha\beta} means for fixed \alpha or fixed \beta. You could put other conserved quantities in some tensor T; the divergence of one of the indices means then covariant conservation of that quantity.
 

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