Parallel transport approximation

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SUMMARY

The discussion centers on the parallel transport equation, specifically the equation represented as \(\frac{d\lambda^{\mu}}{d\tau} = -\Gamma^{\mu}_{\sigma\rho} \frac{dx^{\sigma}}{d\tau} \lambda^{\rho}\). The user explores the validity of deriving the second derivative with respect to tau, leading to a more complex expression involving Christoffel symbols. The user seeks confirmation on whether their approach to parallel transport over small distances is correct, having previously encountered errors in their calculations but currently feeling confident in their methodology.

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  • Understanding of differential geometry and the role of Christoffel symbols
  • Familiarity with the concept of parallel transport in curved spaces
  • Knowledge of calculus, particularly derivatives and Taylor series expansions
  • Experience with tensor notation and manipulation
NEXT STEPS
  • Study the derivation and applications of the parallel transport equation in general relativity
  • Learn about the significance of Christoffel symbols in geodesic equations
  • Explore Taylor series expansions and their use in approximating functions in physics
  • Investigate common pitfalls in calculations involving parallel transport and curvature
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Mathematicians, physicists, and students studying general relativity or differential geometry, particularly those interested in the applications of parallel transport in curved spaces.

jostpuur
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The parallel transport equation is

<br /> \frac{d\lambda^{\mu}}{d\tau} = -\Gamma^{\mu}_{\sigma\rho} \frac{dx^{\sigma}}{d\tau} \lambda^{\rho}<br />

If I take the derivative of this with respect to tau, and get

<br /> \frac{d^2\lambda^{\mu}}{d\tau^2} = -\partial_{\nu}\Gamma^{\mu}_{\sigma\rho}\frac{dx^{\nu}}{d\tau}\frac{dx^{\sigma}}{d\tau} \lambda^{\rho} \;- \;\Gamma^{\mu}_{\sigma\rho}\frac{d^2x^{\sigma}}{d\tau^2}\lambda^{\rho} \;-\; \Gamma^{\mu}_{\sigma\rho}\frac{dx^{\sigma}}{d\tau}\frac{d\lambda^{\rho}}{d\tau}<br />
<br /> = \Big(-\partial_{\nu}\Gamma^{\mu}_{\sigma\rho} \frac{dx^{\nu}}{d\tau}\frac{dx^{\sigma}}{d\tau} \; - \;\Gamma^{\mu}_{\sigma\rho}\frac{d^2x^{\sigma}}{d\tau^2}\;+\; \Gamma^{\mu}_{\sigma\nu}\Gamma^{\nu}_{\alpha\rho} \frac{dx^{\sigma}}{d\tau}\frac{dx^{\alpha}}{d\tau}\Big)\lambda^{\rho}<br />

and then substitute these into

<br /> \lambda^{\mu}(\tau) = \lambda^{\mu}(0) \;+\; \tau\frac{d\lambda^{\mu}(0)}{d\tau} \;+\; \frac{1}{2}\tau^2\frac{d^2\lambda^{\mu}(0)}{d\tau^2} \;+\; O(\tau^3}),<br />

have I already done something wrong, or is this a valid way to do parallel transport small distances?
 
Last edited:
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I was getting wrong answers in one exercise, and started doubting this, but I located the mistake (or a mistake), and right now I have no particular reason to believe that there was anything wrong in this.
 

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