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!