What is the covariant derivative of the position vector?

In summary: It corresponds to the vector length of the path. The covariant derivative of the position vector $\vec R$ is just the vector length of the path's directional derivative.
  • #1
Alain De Vos
36
1
What is the covariant derivative of the position vector $\vec R$ in a general coordinate system?
In which cases it is the same as the partial derivative ?
 
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  • #2
In a general manifold there is no such thing as a position vector.

The partial derivative is equivalent to the covariant derivative only when the connection coefficients vanish.
 
  • #3
In the old context (no differential manifolds etc.) the question does not make sense either because the coordinates ##x^i## are not contravariant vectors.
 
  • #4
Indeed, the upper index on coordinates can be very deceiving. The coordinates ##x^i## (with ##i=1,2,\ldots,n##) do NOT define a vector, but a collection of n scalar functions from your manifold to ##R^n##!

What can be defined, is e.g. a curve on the manifold with a directional derivative, which is a vector.
 
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  • #5
haushofer said:
do NOT define a vector, but a collection of n scalar functions from your manifold to ##R^n##!
What if one re-defines them such that they are components of a vector... but I know, such thing would be useless because they would lose they meaning as coordinates..
 
  • #7
Alain De Vos said:
What is the covariant derivative of the position vector $\vec R$ in a general coordinate system?
In which cases it is the same as the partial derivative ?

As Orudruin says, position is not a vector in curved space. Think about the surface of the Earth. New York has a position. London has a position. What does it mean to vectorially add those positions?

What does always make sense is a tangent vector to a parametrized path. If ##\mathcal{P}(s)## is a path through your space parameterized by some real number ##s## (for example, the position on the Earth of a traveler as a function of the time on his watch), then the quantity ##\frac{d\mathcal{P}}{ds}## is always a vector.
 

What is the covariant derivative of the position vector?

The covariant derivative of the position vector is a mathematical tool used in differential geometry to describe how a vector changes as it moves along a curved surface. It takes into account the curvature of the surface and the orientation of the vector.

How is the covariant derivative of the position vector calculated?

The covariant derivative of the position vector is calculated using the Christoffel symbols, which are derived from the metric tensor of the surface. These symbols represent the connection between the tangent spaces at different points on the surface.

What is the importance of the covariant derivative of the position vector?

The covariant derivative of the position vector is important in many areas of physics, including general relativity, electromagnetism, and fluid dynamics. It allows for the description of how vectors change in curved spaces, which is necessary for understanding many physical phenomena.

How does the covariant derivative of the position vector differ from the ordinary derivative?

The covariant derivative takes into account the curvature of the surface, while the ordinary derivative does not. This means that the covariant derivative of a vector may differ from the ordinary derivative, even if the vector is defined on a flat surface.

Can the covariant derivative of the position vector be generalized to higher dimensions?

Yes, the covariant derivative of the position vector can be generalized to higher dimensions. In three-dimensional space, it is known as the Levi-Civita connection, and in higher dimensions, it is known as the Riemannian connection.

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