Special relativity: components of a metric tensor

[Uku]

Homework Statement

An interval in Minkovski space is given in spheric coordinates as;

$$ds^{2}=c^{2}dt^{2}-dr^{2}-r^{2}d\theta^{2}-r^{2}sin^{2}\theta d\phi^{2}$$

Now I have to find the covariant and contravariant components of the metric tensor.

Homework Equations

General expression of a metric tensor is:
$$G=g_{\mu\nu}dx^{\mu}dx^{\nu}$$ which also equals $$ds^{2}$$

The Attempt at a Solution

I have some messy answer written down from the lecture, but can't get it clear.
Seems that I have written down the covariant components of the metric as
$$g_{00}=1$$
$$g_{11}=-1$$
$$g_{22}=-r^{2}$$
$$g_{33}=-r^{2}sin^{2}\theta$$
Are these the covariant components that the problem asks me to find? How are they found?

I see a correlation in the Schwarzschild metric

G=[PLAIN]http://rqgravity.net/images/gravitation/Gravitation-92.gif

After this it seems that the lecturer has written down that

$$g_{\mu\sigma} g^{\mu\rho}=\delta^{\rho}_{\sigma}$$

Is this correct?

So I get a matrix on which all the components on the main diagonal are 1. From there I can derive that the contra-variant components of the metric are simply inverses of the above covariant metric.

 

[vela]

If you expand the implied summations in [itex]ds^2 = g_{\mu\nu} dx^\mu dx^\nu[/tex], you get<br /> <br /> $$ds^2 = g_{00} dx^0 dx^0 + g_{01}dx^0dx^1 + \cdots + g_{32}dx^3dx^2 + g_{33}dx^3dx^3$$<br /> <br /> Keeping in mind that $x^0 = t$, $x^1 = r$, $x^2 = \theta$, and $x^3 = \phi$, compare that expression to <br /> <br /> $$ds^2 = dt^2 - dr^2 - r^2 d\theta^2 - r^2\sin^2\theta\,d\phi^2$$<br /> <br /> You can just read off the components of $g_{\mu\nu}$.<br /> <br /> Your notes are correct in that $g_{\mu\sigma}g^{\mu\rho}=\delta^\rho_\sigma$. Consider<br /> <br /> $$x_\rho = g_{\rho\sigma} x^\sigma=g_{\rho\sigma}g^{\sigma\mu}x_\mu$$<br /> <br /> You can see that all $g_{\rho\sigma}g^{\sigma\mu}$ does is change the label of the index on $x_\mu$. In other words, it's just the identity.[/itex]

 

[Uku]

Thanks!

A well, actually I have a question still.
The bit:

$$ds^{2}=g_{\mu\nu}dx^{\mu} dx^{\nu}$$

indicates summation over 16 (4x4) values, yes? With only the main diagonal being significant on the g.

EDIT: yes, that is what happens.