Covariant derivative only for tensor

In summary: Another way to say this is that the covariant derivative is a connection that defines a tensor field as a function of a displacement vector.
  • #1
mertcan
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Hi initially I am aware that christoffel symbols are not tensor so their covariant derivatives are meaningless, but my question is why do we have to use covariant derivative only with tensors? ?? Is there a logic of this situation? ?
 
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  • #2
I think there's more than one possible explanation. One of them is that by construction the covariant derivative measures the change of a vector in a given displacement. This is so by construction and by definition, i.e. we want to construct the derivative of a vector and we want to do so in analogy with case of funtions (construction), which is the limit of the difference of the vectors two points when the distance comes to zero, therefore it should be a vector too.

If you want to see the change of functions, you just use the ordinary derivative.
 
  • #4
mertcan said:
but my question is why do we have to use covariant derivative only with tensors? ?? Is there a logic of this situation? ?
If you do not, the result will not be invariant.

Since you labeled this thread "A": A priori, a tensor field is a section over the corresponding tensor bundle. Since the tensors at different points of the base manifold belong to different tensor spaces. As you will remember from basic calculus, derivatives were defined by taking differences of functions at different points and studying how it behaves as those points approach each other. However, for tensor fields there is a priori no natural way of taking differences of tensors at different points of the manifold and in order to be able to define a derivative we therefore must introduce a connection that can be used to relate the tensor spaces at different points to each other. This connection defines the covariant derivative and it makes no sense to talk about the "ordinary" derivative because it is unclear what it would mean.
 
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Related to Covariant derivative only for tensor

1. What is a covariant derivative in tensor calculus?

A covariant derivative is a mathematical operation that extends the concept of a derivative to tensor fields. It measures how a tensor field changes as one moves along a given direction in a curved space.

2. How is a covariant derivative different from a regular derivative?

A regular derivative only takes into account the changes of a function in the direction of the chosen coordinate system, while a covariant derivative takes into account the changes of a tensor field in the direction of a curved space.

3. Why is a covariant derivative important in tensor calculus?

A covariant derivative allows for the differentiation of tensor fields in curved spaces, which is essential for many scientific fields such as general relativity and fluid dynamics. It also helps to define geometric quantities that are independent of the coordinate system used.

4. How is a covariant derivative calculated?

The calculation of a covariant derivative involves using the Christoffel symbols, which represent the curvature of the space, and the partial derivatives of the tensor field with respect to the chosen coordinate system. These values are then combined to give the covariant derivative of the tensor field.

5. Can a covariant derivative be applied to all types of tensors?

Yes, a covariant derivative can be applied to all types of tensors, including scalars, vectors, and higher-order tensors. However, the formula for calculating the covariant derivative will vary depending on the type of tensor being differentiated.

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