- #1
Ron19932017
- 32
- 3
I wonder how an object, like our sun, can approach a more perfect blackbody.
We know that by the wiki definition, blackbody is something that absorb all radiation and is in thermal equilibrium. Its spectrum only depends on T.
We also know that, our Sun's spectrum is blackbody like, while a galaxy/nebula's spectrum is not. I heard explanations like we require the gas to be dense to be a blackbody. That's where my confusion comes.
1.) Suppose our sun is twice denser, does that means it more blackbody-like? and why?
2.) Except from the emission/absorption line, our Sun's continuous spectrum is offset from a perfect blackbody. Is this discrepency due to the density of the Sun not high enough?
3.) Does hot diffuse gas have emission lines, plus a non-blackbody-like continuous spectrum? I wonder how one can calculate that non-blackbody-like continuous spectrum, assuming the diffuse gas is in thermal equalibrium.
We know that by the wiki definition, blackbody is something that absorb all radiation and is in thermal equilibrium. Its spectrum only depends on T.
We also know that, our Sun's spectrum is blackbody like, while a galaxy/nebula's spectrum is not. I heard explanations like we require the gas to be dense to be a blackbody. That's where my confusion comes.
1.) Suppose our sun is twice denser, does that means it more blackbody-like? and why?
2.) Except from the emission/absorption line, our Sun's continuous spectrum is offset from a perfect blackbody. Is this discrepency due to the density of the Sun not high enough?
3.) Does hot diffuse gas have emission lines, plus a non-blackbody-like continuous spectrum? I wonder how one can calculate that non-blackbody-like continuous spectrum, assuming the diffuse gas is in thermal equalibrium.
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