# View of the sky from inside a black hole

Consider an observer located at radius $r_o$ from a Schwarzschild black hole of radius $r_s$. The observer may be inside the event horizon ($r_o < r_s$).

Suppose the observer receives a light ray from a direction which is at angle $\alpha$ with respect to the radial direction, which points outward from the black hole.

What is the original, incident angle of the light ray $\varphi$ from infinity? That is, if we were to trace the light ray back through time, which point on the celestial sphere did it come from?

See the diagram below:

According to this source, we have

$$\varphi = \int_{r_o}^\infty \frac{\mathrm{d}r}{r^2 \sqrt{ \frac{1}{b^2} - \frac{1}{r^2} \left(1-\frac{r_s}{r}\right) }}$$

where $b$ is the impact parameter, which is the distance between the ray at infinity and a ray parallel to it that plunges directly into the black hole. The impact parameter is given here as

$$b = m c \frac{h}{E} = m c r^2 \frac{\mathrm{d}\varphi}{\mathrm{d}\tau} \frac{1}{mc^2} \frac{\mathrm{d}\tau}{\mathrm{d}t} \left(1 - \frac{r_s}{r}\right)^{-1} = \frac{r^2}{c} \left( 1 - \frac{r_s}{r} \right)^{-1} \frac{\mathrm{d}\varphi}{\mathrm{d}t}$$

taking $r = r_o$. Therefore

$$\frac{1}{b^2} = \frac{c^2}{r^4} \left( 1 - \frac{r_s}{r} \right)^2 \left( \frac{\mathrm{d}t}{\mathrm{d}\varphi} \right)^2$$

To find the last term, recall that the metric is given by

$$0 = \left( 1- \frac{r_s}{r} \right) c^2 \mathrm{d}t^2 - \left( 1- \frac{r_s}{r} \right)^{-1} \mathrm{d}r^2 - r^2 \mathrm{d}\varphi^2$$

for a light ray. Dividing by $\mathrm{d}\varphi^2$ yields

\begin{align} 0 &= \left( 1- \frac{r_s}{r} \right) c^2 \left(\frac{\mathrm{d}t}{\mathrm{d}\varphi}\right)^2 - \left( 1- \frac{r_s}{r} \right)^{-1} \left(\frac{\mathrm{d}r}{\mathrm{d}\varphi}\right)^2 - r^2 \\ \left( 1- \frac{r_s}{r} \right) c^2 \left(\frac{\mathrm{d}t}{\mathrm{d}\varphi}\right)^2 &= \left( 1- \frac{r_s}{r} \right)^{-1} \left(\frac{\mathrm{d}r}{\mathrm{d}\varphi}\right)^2 + r^2 \\ c^2 \left(\frac{\mathrm{d}t}{\mathrm{d}\varphi}\right)^2 &= \left( 1- \frac{r_s}{r} \right)^{-2} \left(\frac{\mathrm{d}r}{\mathrm{d}\varphi}\right)^2 + r^2 \left( 1- \frac{r_s}{r} \right)^{-1} \\ \left(\frac{\mathrm{d}t}{\mathrm{d}\varphi}\right)^2 &= \frac{1}{c^2} \left( 1- \frac{r_s}{r} \right)^{-2} \left(\frac{\mathrm{d}r}{\mathrm{d}\varphi}\right)^2 + \frac{r^2}{c^2} \left( 1- \frac{r_s}{r} \right)^{-1} \end{align}

Hence

\begin{align} \frac{1}{b^2} &= \frac{c^2}{r^4} \left( 1 - \frac{r_s}{r} \right)^2 \left( \frac{1}{c^2} \left( 1- \frac{r_s}{r} \right)^{-2} \left(\frac{\mathrm{d}r}{\mathrm{d}\varphi}\right)^2 + \frac{r^2}{c^2} \left( 1- \frac{r_s}{r} \right)^{-1} \right) \\ &= \frac{1}{r^4} \left( \left(\frac{\mathrm{d}r}{\mathrm{d}\varphi}\right)^2 + r^2 \left( 1- \frac{r_s}{r} \right) \right) \\ &= \frac{1}{r^4} \left(\frac{\mathrm{d}r}{\mathrm{d}\varphi}\right)^2 + \frac{1}{r^2} \left( 1- \frac{r_s}{r} \right) \end{align}

The relationship between $\mathrm{d}\varphi$ and $\mathrm{d}r$ can be derived as follows:

$$\tan \alpha = r \frac{\mathrm{d}\varphi}{\mathrm{d}r}$$

$$\frac{\mathrm{d}\varphi}{\mathrm{d}r} = \frac{\tan \alpha}{r}$$

$$\left(\frac{\mathrm{d}r}{\mathrm{d}\varphi}\right)^2 = r^2 \cot^2 \alpha$$

Therefore

\begin{align} \frac{1}{b^2} &= \frac{1}{r^4} r^2 \cot^2 \alpha + \frac{1}{r^2} \left( 1- \frac{r_s}{r} \right) \\ &= \frac{1}{r^2} \cot^2 \alpha + \frac{1}{r^2} \left( 1 - \frac{r_s}{r} \right) \\ &= \frac{1}{r^2} \left( \cot^2 \alpha + 1 - \frac{r_s}{r} \right) \\ &= \frac{1}{r^2} \left( \csc^2 \alpha - \frac{r_s}{r} \right) \end{align}

and thus

$$\varphi = \int_{r_o}^\infty \frac{\mathrm{d}r}{r^2 \sqrt{ \frac{1}{r_o^2} \left( \csc^2 \alpha - \frac{r_s}{r_o} \right) - \frac{1}{r^2} \left(1-\frac{r_s}{r}\right) }}$$

Is this expression correct? Is there a closed form in terms of elliptic functions or other special functions?

• Why do you ask? Your reference on PG coordinates has the graphic. Not that I believe it, but why do you want more, and since you seem to know where to find how to do it, why ask here? Or are you asking if there is anything wrong with the description you referenced? Jul 3, 2016 at 2:15
• @BobBee The reference gives neither the value of $I$ nor the final expression (if there is a closed form). Jul 3, 2016 at 2:31
• Well, somebody has to work it through. Have you given it a try? Jul 3, 2016 at 2:42
• This seems like a homework problem What have you tried to solve it? Jul 3, 2016 at 7:58
• @RobJeffries This is not a homework problem. I have updated the question with more details. Jul 3, 2016 at 15:10