Coordinate transformation of contravariant vectors.

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SUMMARY

The coordinate transformation of contravariant vectors is accurately represented by the equation V'a=(dX'a/dXb)Vb, where the indices a and b are essential for indicating the relationship between components during transformation. The discussion clarifies that using a single index, as in V'a=(dX'a/dXa)Va, incorrectly implies that each component of the transformed vector solely depends on its corresponding component of the original vector. This misunderstanding is addressed by emphasizing the necessity of summation over all components, as indicated by the second index, which is crucial for accurate representation in tensor calculus.

PREREQUISITES
  • Understanding of contravariant vectors
  • Familiarity with tensor calculus
  • Knowledge of partial derivatives
  • Basic grasp of coordinate transformations
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  • Study the properties of contravariant and covariant vectors
  • Learn about the Einstein summation convention in tensor notation
  • Explore coordinate transformation equations in differential geometry
  • Investigate applications of tensor calculus in physics
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This discussion is beneficial for physicists, mathematicians, and students studying advanced topics in vector calculus and differential geometry, particularly those focusing on the transformation properties of tensors.

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Note: The derivatives are partial.

I've seen the coordinate transformation equation for contravariant vectors given as follows,

V'a=(dX'a/dXb)Vb

What I don't get is the need for two indices a and b. Wouldn't it be adequate to just write the equation as follows?

V'a=(dX'a/dXa)Va

The prime being adequate to indicate the new and the unprimed the old, coordinates and contravariant vector. Or does the second index provide some more information which I am unaware of?
 
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The first equation has on the LHS a single component of V' while the RHS is a sum by summation convention over all the unprimed components.
V&#039;^1 = \frac{\partial X&#039;^1}{\partial X^1}V^1 + \cdots + \frac{\partial X&#039;^1}{\partial X^n}V^n\\<br /> \vdots<br /> V&#039;^m = \frac{\partial X&#039;^m}{\partial X^1}V^1 + \cdots + \frac{\partial X&#039;^m}{\partial X^n}V^n<br />
Your equation is a single component and represents no sum, so it is not equivalent.
V&#039;^1 = \frac{\partial X&#039;^1}{\partial X^1}V^1<br /> \vdots<br /> V&#039;^m = \frac{\partial X&#039;^m}{\partial X^m}V^m
It seems to state that the ath component of V' depends only on the ath component of V, which is usually not the case.
 
Last edited:
Ok thanks, that makes sense now.
 

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