1
$\begingroup$

I have the following cosmology exercise:

i) calculate the evolution scale factor for an open empty universe and write down its spacetime metric in terms of coordinate $\chi$ \begin{equation} d\chi = \frac{dr}{\sqrt{1-Kr^2}}. \end{equation}

ii) show that this is equivalent to the Minkowski metric $$ds^2 = d\tau^2 -dr^2 -r^2d\Omega^2 $$ using the following transformation: $$\tau=t \text{cosh}(|k|^{1/2}\chi) \quad \text{and} \quad r = t \text{sinh}(|k|^{1/2}\chi).$$

For i) I computed the scale factor from the I Friedman equation with $\Lambda = \rho = 0 $ for a empty universe:

\begin{equation} a(t)=\int \dot{a}(t) dt= \int_0^t c dt = [ct]^t_0=ct_o \end{equation}

where the metric is a Roberston-Walker metric:

\begin{eqnarray} ds^2&=&(cdt)^2 -a^2(t)\bigg (\frac{dr^2}{1-Kr^2} + r^2d\Omega^2 \bigg) \\ &=&(cdt)^2 -a^2(t)\bigg (d\chi^2 + S_k(r)^2d\Omega^2 \bigg) \end{eqnarray}

is that correct?

For the ii) However I have no ideas.. I noticed that the Minkowsi metric is given in spherical coordinate but I don't understand how to do the transform. Could anyone help me?

I just tried to derive the given coordinate and replace the result in Minkowski metric formula in order to obtain the RW metric but its not working...

\begin{equation} dr=dt \text{sinh}(\sqrt{|k|}\chi) + t \text{cosh}(\sqrt{|k|}\chi) \sqrt{|k|} d\chi \end{equation}

\begin{equation} d\tau=dt \text{cosh}(\sqrt{|k|}\chi) + t \text{sinh}(\sqrt{|k|}\chi) \sqrt{|k|} d\chi \end{equation}

$\endgroup$
2
  • $\begingroup$ Your metric needs to be written in terms of $χ$ only with no mention of $r$. Also, $a(t)$ needs to be unitless since $χ$ has units of length. See if those fixes solve your problem. $\endgroup$
    – benrg
    Nov 27, 2020 at 18:19
  • $\begingroup$ Yeah I think this fixed the problem ! thanks:) What do you mean with a(t) has to be unitless ? $\endgroup$
    – Apinorr
    Nov 28, 2020 at 10:02

1 Answer 1

0
$\begingroup$

So I think that my problem was that I forgot to replace $r=t\text{sinh}(\sqrt{|k|}\chi)$ in my Minkowski metric ! But after replacing it, and replacing the derivative I kind of get the Robertson-Walker metric again, with $a(t)=t$ and with $S_k(r)=R\text{sinh}(\frac{\chi}{R})$ for an open universe. I don't know if this can help anyone but I just let the post here in case :)

$\endgroup$

Your Answer

By clicking “Post Your Answer”, you agree to our terms of service and acknowledge that you have read and understand our privacy policy and code of conduct.

Not the answer you're looking for? Browse other questions tagged or ask your own question.