Riemannian Manifold: Integral Formula Explained

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SUMMARY

The discussion focuses on the integral formula for Riemannian manifolds, specifically the expression integral from 0 to T of sqrt(g_ij c'(t) c'(t)). Here, g_ij represents the metric tensor, and c'(t) denotes the tangent vector to the curve c(t). The implementation involves premultiplying and postmultiplying the metric tensor matrix by the tangent vector to obtain a scalar value, exemplified using the standard Euclidean metric in R2. The resulting expression illustrates how different metrics yield varying notions of length.

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whattttt
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Can someone please explain to me how this formula
integral from 0 to T of
sqrt(g_ij c'(t) c'(t))
I have seen it on wikipedia but don't know how to actually implement the formula.
 
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(g_ij) is the metric tensor, c'(t) is, for each t, a tangent vector to the curve c(t).
With respect to a specific choice of coordinates, (g_ij) is a matrix that you premultiply and postmultiply by c'(t) to get a scalar. For example, the standard Euclidean metric in R2 with Cartesian coordinates is
\left(\begin{array}{cc}1 & 0\\0 & 1\end{array}\right)
A typical curve in 2-dimensional Euclidean space with Cartesian coordinates has tangent vector
c'(t) = \left(\begin{array}{c}\frac{dx}{dt}\\ \frac{dy}{dt}\end{array}\right)
Premultiplying and postmultiplying gets us the expression:
\left(\begin{array}{cc}\frac{dx}{dt} & \frac{dy}{dt}\end{array}\right) \left(\begin{array}{cc}1 & 0\\0 & 1\end{array}\right) \left(\begin{array}{c}\frac{dx}{dt}\\ \frac{dy}{dt}\end{array}\right)
= \left(\frac{dx}{dt}\right)^2 + \left(\frac{dy}{dt}\right)^2
Different metrics will give different notions of length.
 

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