What Does 'To Lowest Order' Mean in the Derivation of Riemann Curvature Tensor?

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SUMMARY

The discussion centers on the interpretation of the phrase "to lowest order" in the derivation of the Riemann curvature tensor, specifically the transition between equations 89 and 97 in the context of General Relativity (GR). The participants highlight the use of the Fundamental Theorem of Calculus and a truncated Taylor expansion to understand the changes in components when parallel transported. The conversation emphasizes the mathematical theorem that allows the interchange of differentiation and integration, leading to the derivation of the Riemann curvature tensor from the previous equations.

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  • Familiarity with the Fundamental Theorem of Calculus
  • Knowledge of Taylor series expansions
  • Basic principles of tensor calculus
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This discussion is beneficial for students and researchers in physics, particularly those studying General Relativity, as well as mathematicians interested in the application of calculus in theoretical physics.

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http://www.mth.uct.ac.za/omei/gr/chap6/frame6.html" is a derivation of the components of the riemann curvature tensor. the problem is that i can't understand the transition between eq97 and eq89 .
what does "To lowest order " mean ?
 
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I'm not familiar at all with the notation (GR tends to have the most horrible formulas I've ever seen), but the first step looks like a use of the Fundamental Theorem of Calculus, and the approximation looks like some sort of truncated Taylor expansion.
 
Hi, just found your question today. I am working through Dunsby's webpages which are almost identical to Schutz's" Introduction to General relativity". Ok , my understanding of eqns 92 to 97 are...
He finds the change in the component V alpha when parallel transported around the loop to get eqn 97. The each pair of terms has the form... integral @ x=a + delta a MINUS integral @ x= a. This is just like delta f = df/ dx . delta x to first order .
i take it there is some mathematical theorem that allows you to change d/dx of an integral into an integral of d/dx ... giving eqn 98.
then using eqn 99 or 92 again we arrive at the Riemann curvature tensor

PS. Does anyone else find that web pages and lecture notes on GR are poorly explained and very difficult to work through unaided? I've self- studied Maths to degree level using OU courses and always found the reasoning well explained. BUT not GR!
Cheers!
 

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