Geodesic in 2D Space: Understanding the Statement

[vidi]

Homework Statement

I am having trouble understanding how the following statement (taken from some old notes) is true:

>For a 2 dimensional space such that ds^2=\frac{1}{u^2}(-du^2+dv^2)
the timelike geodesics are given by u^2=v^2+av+b where a,b are constants.

Homework Equations

Euler-Lagrange, Normalisation condition

The Attempt at a Solution

When I see "geodesics" I jump to the Euler-Lagrange equations. They give me
\frac{d}{d\lambda}(-2\frac{\dot u}{u^2})=(-\dot u^2+\dot v^2)(-\frac{2}{u^3})\\<br /> \implies \frac{\ddot u}{u^2}-2\frac{\dot u^2}{u^3}=\frac{1}{u^3}(-\dot u^2+\dot v^2)\\<br /> \implies u\ddot u-\dot u^2-\dot v^2=0
and
\frac{d}{d\lambda}(2\frac{\dot v}{u^2})=0\\<br /> \implies \dot v=cu^2
where c is some constant.

Timelike implies \dot x^a\dot x_a=-1 where I have adopted the (-+++) signature.

I can't for the life of me see how the statement results from these. Would someone mind explaining? Thanks.

 

[Thaakisfox]

Do not expand the Euler-Lagrange equations. But do a trick like this:

The Lagrangian is:

L = \frac{1}{u}\sqrt{\left(\frac{dv}{du}\right)^2-1}= \frac{1}{u}\sqrt{v&#039;^2-1}

Now you see this doesn't depend on $v$. The Euler Lagrange equations then give:

0=\frac{\partial L}{\partial v}=\frac{d}{du}\frac{\partial L}{\partial v&#039;} \Longrightarrow \frac{\partial L}{\partial v&#039;}=C

Now calculate \frac{\partial L}{\partial v&#039;} from the Lagrangian and put it equal to the constant C. This will lead to a differential equation which gives the solution you were looking for.

 

[vidi]

Thanks, Thaakisfox, I've got it now!