What is the covariant derivative of the position vector?

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Discussion Overview

The discussion revolves around the covariant derivative of the position vector in a general coordinate system, particularly in the context of differential geometry and manifolds. Participants explore the conditions under which the covariant derivative may coincide with the partial derivative and the implications of defining position vectors in curved spaces.

Discussion Character

  • Exploratory
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • One participant questions the covariant derivative of the position vector $\vec R$ and seeks clarification on when it is equivalent to the partial derivative.
  • Another participant asserts that in a general manifold, the concept of a position vector does not exist, and the covariant derivative equals the partial derivative only when the connection coefficients vanish.
  • A further contribution emphasizes that in traditional contexts, coordinates are not contravariant vectors, which complicates the question of the covariant derivative.
  • It is noted that coordinates can be misleading, as they represent scalar functions rather than vectors, and that a directional derivative can be defined for curves on the manifold.
  • A participant speculates about redefining coordinates as components of a vector but acknowledges the potential loss of meaning in doing so.
  • Another participant expresses uncertainty regarding the implications of redefining coordinates.
  • A later reply reiterates the initial question about the covariant derivative and highlights that position is not a vector in curved space, using the example of geographical locations like New York and London. It emphasizes that tangent vectors to parametrized paths are always well-defined.

Areas of Agreement / Disagreement

Participants do not reach a consensus; multiple competing views remain regarding the nature of position vectors and the conditions under which the covariant derivative aligns with the partial derivative.

Contextual Notes

The discussion reveals limitations in understanding the relationship between coordinates and vectors in curved spaces, as well as the implications of defining derivatives in such contexts. There is an unresolved tension between traditional and modern interpretations of these concepts.

Alain De Vos
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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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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.
 
In the old context (no differential manifolds etc.) the question does not make sense either because the coordinates ##x^i## are not contravariant vectors.
 
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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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..
 
I'm not sure what that would mean.
 
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.
 

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