weirdoguy
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happyparticle said:I think this is what I'm looking for
No you're not. And again: from which textbook did you get this exercise? Autors name, and the name of the book please.
happyparticle said:I think this is what I'm looking for
I didn't get this exercise from a textbook. This exercise is one of multiple exercises I found to get used with the Scharwarzshield metric. I tought this problem would be a good practice. However, it is possible that I just don't understand the question.weirdoguy said:No you're not. And again: from which textbook did you get this exercise? Autors name, and the name of the book please.
But where precisely was it "found"? Or did you invent the exercise yourself?happyparticle said:This exercise is one of multiple exercises I found to get used with the Scharwarzshield metric. I tought this problem would be a good practice.
ViXra is a well-known crackpot site. You should not trust material posted there. Correspondingly, what you just said is nonsense.happyparticle said:I didn't get this exercise from a textbook. This exercise is one of multiple exercises I found to get used with the Scharwarzshield metric. I tought this problem would be a good practice. However, it is possible that I just don't understand the question.
It is possible that the density of the black hole is $$\rho = \frac{3}{32 \pi} \frac{c^6}{G^3 M^2}$$ as explained [vixra link], meaning that the volume is "simply" $$V = \frac{4 \pi}{3 r_s^3}$$. Which makes sense in my opinion. ##r_s## is the radius of Scharwarzshield, which is the radius at the horizon of the black hole. Hence, $$V = \frac{4 \pi}{3 r_s^3}$$ would be the volume of the black hole. However, I'm not sure how to get this expression from the Scharwarzshield metric.
It would have saved a lot of time if you had given this reference at the start of the thread--as you're supposed to do anyway for a homework thread.happyparticle said:as explained here,