by dougettinger » Fri Apr 22, 2011 3:18 pm
Ann wrote:Why do different elements become ionized at different distances from a star? Does each element as you see it farther from a star need less UV and less heat to be ionized ?
The way I understand it, nitrogen requires less UV than hydrogen to become ionized, and therefore ionized nitrogen will typically be found farther from the central star of a planetary nebula than ionized hydrogen. Check out this link:
http://apod.nasa.gov/apod/ap090122.html
When it comes to oxygen, it can only become ionized in very rarefied conditions, so that you won't see oxygen emission inside dust clouds, for example. Ann
My understanding is that for very massive stars, each subsequent core collapse should produce the following elements starting with the first core collapse: H, He, C with some N, Ne, O with some Mg, Si with some S, and finally Fe with some Ni. Of course, for less massive stars this chain of fused elements does not go as far as iron. For our Sun, supposely, it should only collapse once or twice to produce H, He, and perhaps C with some N.
The elements as they are expelled from the various core collapses, will start cooling because they are moving farther away from the heat of the remaining star, and because the longer time they move away the ionization energy is lost due to radiant heat transfer. For the first nth ionization energies the above elements require the following descending energies. As these elements move farther away from the star and time, t, for their respective expolsion they will continually lose ionization energy. Those desending energies are 2372 kJ/mol for He, 2080 for Ne, 1402 for N, about 1312 for H and O, about 1040 for C and S, and about 770 for Fe and Si.
Knowing these facts, assuming that they are logical and correct, one can analyze the planetary nebula NGC 2818, 4 ly in diameter, that you have referenced. The source star has already imploded at least 5 times for H, He, C, Ne, and O since ionization of O can be readily observed. During the explosion for carbon, some nitrogen was produced which one can still observe because the ionization energies have not dropped below 1402 kJ/mol. Some hydrogen is always emitted with each explosion and can be observed because the its ionization energy is below 1402 kJ/mol. Helium was the second element expelled and cannot be detected because it has cooled below its ionization energy of 2372. Neon, the third element to be expelled, cannot be detected because it also has cooled below it very high ionization energy of 2080.
The shock front for the explosion that created oxygen has already caught up to the shock front that produced Ne and C since the nitrogen that was produced in the carbon explosion is observed to be farther from the source star than oxygen. This indicates that later shock fronts accelerate faster than shock fronts from previous explosions.
Ann, I hope you can undertand this petit dissertation. I am not sure that it is completely correct. You have been very helpful in explaining the detection of the different elements from the colors that are recorded. I hope to solicit more of your commentary and also any criticisms from expert star evolutionists.
I used Wikepedia's stellar evolution, ionization energy, and the various elements as some of my references.
[quote="Ann"][quote]Why do different elements become ionized at different distances from a star? Does each element as you see it farther from a star need less UV and less heat to be ionized ? [/quote]
The way I understand it, nitrogen requires less UV than hydrogen to become ionized, and therefore ionized nitrogen will typically be found farther from the central star of a planetary nebula than ionized hydrogen. Check out this link:
[url]http://apod.nasa.gov/apod/ap090122.html[/url]
When it comes to oxygen, it can only become ionized in very rarefied conditions, so that you won't see oxygen emission inside dust clouds, for example. Ann[/quote]
My understanding is that for very massive stars, each subsequent core collapse should produce the following elements starting with the first core collapse: H, He, C with some N, Ne, O with some Mg, Si with some S, and finally Fe with some Ni. Of course, for less massive stars this chain of fused elements does not go as far as iron. For our Sun, supposely, it should only collapse once or twice to produce H, He, and perhaps C with some N.
The elements as they are expelled from the various core collapses, will start cooling because they are moving farther away from the heat of the remaining star, and because the longer time they move away the ionization energy is lost due to radiant heat transfer. For the first nth ionization energies the above elements require the following descending energies. As these elements move farther away from the star and time, t, for their respective expolsion they will continually lose ionization energy. Those desending energies are 2372 kJ/mol for He, 2080 for Ne, 1402 for N, about 1312 for H and O, about 1040 for C and S, and about 770 for Fe and Si.
Knowing these facts, assuming that they are logical and correct, one can analyze the planetary nebula NGC 2818, 4 ly in diameter, that you have referenced. The source star has already imploded at least 5 times for H, He, C, Ne, and O since ionization of O can be readily observed. During the explosion for carbon, some nitrogen was produced which one can still observe because the ionization energies have not dropped below 1402 kJ/mol. Some hydrogen is always emitted with each explosion and can be observed because the its ionization energy is below 1402 kJ/mol. Helium was the second element expelled and cannot be detected because it has cooled below its ionization energy of 2372. Neon, the third element to be expelled, cannot be detected because it also has cooled below it very high ionization energy of 2080.
The shock front for the explosion that created oxygen has already caught up to the shock front that produced Ne and C since the nitrogen that was produced in the carbon explosion is observed to be farther from the source star than oxygen. This indicates that later shock fronts accelerate faster than shock fronts from previous explosions.
Ann, I hope you can undertand this petit dissertation. I am not sure that it is completely correct. You have been very helpful in explaining the detection of the different elements from the colors that are recorded. I hope to solicit more of your commentary and also any criticisms from expert star evolutionists.
I used Wikepedia's stellar evolution, ionization energy, and the various elements as some of my references.