Given the metric, find the geodesic equation

whatisreality
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Homework Statement


Given that ##ds^2 = r^2 d\theta ^2 + dr^2## find the geodesic equations.

Homework Equations



The Attempt at a Solution


I think the ##g_{\mu\nu} =
\left( \begin{array}{ccc}
1& 0 \\
0 & r^2 \end{array} \right)##
Then I tried to use the equation
##\tau = \int_{t_1}^{t_2} \sqrt{ g_{\mu\nu}(x(t)) \frac{ dx^{\mu}}{dt}\frac{dx^{\nu}}{dt} } dt##

Which if I expand the sum gives

##\tau = \int_{t_1}^{t_2} \sqrt{ 1 + \left(\frac{ dr}{dt}\right)^2 +r^2 \left(\frac{d\theta}{dt}\right)^2 }## ##dt##

Unfortunately I don't know anything about Lagrangians, which seems to be the normal way to proceed... so I get a bit stuck here. There is an example without Langrangians in the lecture notes but I don't understand what he did to get from here to his ##d\tau##. We've had two lectures on GR so far and I think I've already missed something massively important, that explains how to do this!

Thank you for any help, I really appreciate it. :smile:
 
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whatisreality said:
##\tau = \int_{t_1}^{t_2} \sqrt{ g_{\mu\nu}(x(t)) \frac{ dx^{\mu}}{dt}\frac{dx^{\nu}}{dt} } dt##

Which if I expand the sum gives

##\tau = \int_{t_1}^{t_2} \sqrt{ 1 + \left(\frac{ dr}{dt}\right)^2 +r^2 \left(\frac{d\theta}{dt}\right)^2 }## ##dt##

The one in the square root should not be there. The metric only has two non-zero components and ##t## is a curve parameter, not a coordinate.

What you want to read up on is variational calculus. It will tell you the conditions for a curve to find the extreme values of integrals such as
$$
S = \int_a^b L(x,\dot x,\tau) \, d\tau.
$$
The condition that must be satisfied by ##L## is a differential equation on the form
$$
\frac{\partial L}{\partial x} - \frac{d}{d\tau} \frac{\partial L}{\partial \dot x} = 0,
$$
known as the Euler-Lagrange equation. For its derivation, you should look up any basic textbook containing variational calculus.
 
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