How to calculate the outer product in GR?

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SUMMARY

The discussion focuses on calculating the outer product in the context of General Relativity (GR) using the Fermi-walker transport law. The vectors involved are ##x##, ##y##, ##u##, and ##a##, where ##u## is the tangent vector and ##a = \nabla_u u##. The key equation derived is the change in the dot product along the curve, which ultimately shows that the scalar product remains unchanged. The main challenge highlighted is determining the appropriate spaces for the vectors involved in the outer product calculation.

PREREQUISITES
  • Understanding of Fermi-walker transport in General Relativity
  • Familiarity with tensor notation and operations
  • Knowledge of vector spaces and their properties
  • Basic concepts of differential geometry
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  • Study the properties of the outer product in tensor calculus
  • Explore the implications of Fermi-walker transport on vector fields
  • Learn about the relationship between tangent vectors and their associated spaces
  • Investigate examples of scalar products in differential geometry
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Haorong Wu
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Homework Statement
Show that the scalar product of two vectors is not altered as they are both Fermi-Walker transported along a curve ##C##
Relevant Equations
If a curve is timelike, ##u## is its tangent vector, and ##a=\nabla_u u=Du/d \tau##, then a vector ##V## is said to be Fermi-Walker transported along ##u## if $$ \nabla_u V=(u \otimes a- a \otimes u)\cdot V .$$
I will post the answer here, part of which I do not follow.

Let the two vectors be ##x## and ## y##. Then the Fermi-walker transport law reads$$\nabla_u x=(u \otimes a -a \otimes u) \cdot x$$ $$\nabla_u y=(u \otimes a- a \otimes u)\cdot y ,$$ where ##u## is the tangent vector to the curve ##c## and ##a=\nabla_u u##. Using the product rule we evaluate the change in the dot product along the curve $$\begin{align} \nabla_u ( x \cdot y)&= (\nabla_u x)\cdot y+ x \cdot(\nabla_u y) \nonumber \\& =(a \cdot x) (u \cdot y) -(a \cdot y) (u \cdot x) +(u \cdot x) (a \cdot y) -(a \cdot x) (u \cdot y) =0 . \nonumber \end{align}$$ The scalar product is unaltered.

I do not follow the outer-product part. I know that I should multiply two terms together if they are in the same space. However, in this problem, I do not know how to determin which term belongs to which space. It seems, sometimes ##x## and ##u## are in the same space, and sometimes ##x## and ##a## are in the same space. I am stuck.
 
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By definition, let ##S:= u \otimes a - a \otimes u##, then ##S(\alpha, \beta) = (u \cdot \alpha)(a \cdot \beta) - (a \cdot \alpha)(u \cdot \beta)##
 
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