<p><a href="http://www.sns.ias.edu/~jnb/SNdata/solarmodels.html" rel="noreferrer">A page from the Institute for Advanced Study</a> links to data from various modifications to the Standard Solar Model. The newest given there is from <a href="http://arxiv.org/abs/astro-ph/0412440" rel="noreferrer">Bahcall<sup>1</sup> et al. (2005)</a>, which I'll use as an example. The authors' calculations depend on data from the Opacity project. Data from two models are available through the IAS link: the <a href="http://www.sns.ias.edu/~jnb/SNdata/Export/BS2005/bs05_agsop.dat" rel="noreferrer">BS05(AGS, OP) model</a> and the <a href="http://www.sns.ias.edu/~jnb/SNdata/Export/BS2005/bs05op.dat" rel="noreferrer">BS05(OP) model</a>; the difference lies in the main thing you're interested in: heavy element abundances. BS05(AGS, OP) has, for instance, a central<sup>2</sup> $^{12}\text{C}$ mass fraction of $7.79\times10^{-6}$, while BS05(OP) has a central $^{12}\text{C}$ mass fraction of $1.05\times10^{-5}$. All of the central data from the major thermodynamic variables (e.g. pressure and temperature), as well as the mass fractions, are well within an order of magnitude in each model.</p>

<p>That said, the general heavy element trend is the same in both models. $^{12}\text{C}$ increase by two to three orders of magnitude from the center. $^3\text{He}$ (rather than the more common $^4\text{He}$, which has a mass fraction given by $Y$) increases by one to two orders of magnitude. $^{14}\text{N}$ actually <em>decreases</em> by two orders of magnitude, while $^{16}\text{O}$ remains relatively constant. The model gives no data for silicon.</p>

<p>Other new models agree (though not all), to less than an order of magnitude or so, with the data from Bahcall et al. Graphical representations can be found in e.g. <a href="http://cos.colorado.edu/~kevinf/PAPERS/solmodel.pdf" rel="noreferrer">this paper</a>:</p>

<p><a href="https://i.sstatic.net/aQQm7.png" rel="noreferrer"><img src="https://i.sstatic.net/aQQm7.png" alt="enter image description here"></a></p>

<p>I'm unsure of the reason behind the $^3\text{He}$ spike; that may warrant a follow-up questions. My one guess is that this could be due to its role as an intermediate nucleus in the second step of the <a href="https://en.wikipedia.org/wiki/Proton%E2%80%93proton_chain_reaction" rel="noreferrer">p-p chain</a>. However, the same trends for each element are followed, although the changes in mass fraction are <em>not</em> constant at all radii $r$.</p>

<p>As for your question about how the central figures were derived, the answer is that helioseismological measurements and neutrino fluxes are some of the best indicators of composition. This was used as the basis for the BS05(AGS, OP) and BS05(OP) models, as well as, in fact, most variants of the Standard Solar Model.</p>

<hr>

<p><sup>1 This is Bahcall's page, so, naturally, these are some of his papers. However, the results appear to be consistent with the calculations of others.</sup>
<br>
<sup>2 Technically, this is from about 0.0016 solar radii, but this distance step is comparatively small.</sup></p>

CC BY-SA 3.0
2016-08-03T02:45:48.987Z
Wow, thanks for taking the time to put this together. Those plots are *exactly* what I hoped to see - there's so much happening there! Indeed this suggests further questions. Thank you! The footnotes are appreciated as well, I'm pretty sure John Bahcall's papers can be trusted in this context :-).
uhoh
CC BY-SA 3.0
2016-08-03T03:05:10.627Z
I noticed that there is relatively little overlap between the carbon and nitrogen fraction curves. Might this imply that the CNO cycle is a less common mode of fusion in the Sun?
dualredlaugh
CC BY-SA 3.0
2016-08-03T03:07:59.377Z
@dualredlaugh The CNO cycle is relatively uncommon in the Sun; it starts becoming dominant at about 1.7$\times$10$^7$ K, a bit higher than the Sun's core temperature. So yes, the p-p chain is far more prevalent than the CNO cycle in Sun-like stars.
HDE 226868
CC BY-SA 3.0
2016-08-03T06:57:13.720Z
@dualredlaugh The CNO is energetically unimportant (1%), but *is* responsible for turning almost all the C into N in the core. The N to O (and back to C) bit is much slower.
ProfRob
CC BY-SA 3.0
2016-08-03T00:23:08.427Z
2016-08-03T00:38:21.977Z
2016-08-03T00:38:21.977Z
HDE 226868
<p>In a <a href="https://astronomy.stackexchange.com/q/16707/7982">previous question</a> I asked about the source of carbon and silicate dust that Solar Probe Plus will encounter in its close flyby of the Sun. It seems likely that most sources would include infall from outside the solar system or fragments resulting from collisions inside the solar system.</p>

<p>But the Sun is believed to be about 0.4% carbon and 0.1% silicon by mass (see  <a href="http://hyperphysics.phy-astr.gsu.edu/hbase/tables/suncomp.html" rel="nofollow noreferrer">here</a> and <a href="http://chemistry.about.com/od/geochemistry/a/sunelements.htm" rel="nofollow noreferrer">here</a>). I believe these represent the relative abundances during the formation of the Sun, but do not account for nucleosynthesis that early in the Sun's life.</p>

<p>Is the distribution of carbon and silicon in the Sun is believed to be uniform, or does it have a radially dependent distribution? Is there be any kind of gravitational settling, i.e. heavier atoms tending to move toward the center as happens in planets?</p>

<p>Since we can only directly measure elemental abundances directly near the surface using spectroscopic techniques, would the radial distribution come from some model or calculation?</p>

CC BY-SA 3.0
2016-07-28T21:13:59.217Z
I *believe* what heavier element go to center of core just as it happens with heavier stars.
Free Consulting
<the-sun><elemental-abundances>
How are heavier elements such as carbon and silicon distributed within the Sun?
uhoh
# How are heavier elements such as carbon and silicon distributed within the Sun?

(Asked by: username_0 on 2016-07-26)

In a [previous question](https://astronomy.stackexchange.com/q/16707/7982) I asked about the source of carbon and silicate dust that Solar Probe Plus will encounter in its close flyby of the Sun. It seems likely that most sources would include infall from outside the solar system or fragments resulting from collisions inside the solar system.

But the Sun is believed to be about 0.4% carbon and 0.1% silicon by mass (see [here](http://hyperphysics.phy-astr.gsu.edu/hbase/tables/suncomp.html) and [here](http://chemistry.about.com/od/geochemistry/a/sunelements.htm)). I believe these represent the relative abundances during the formation of the Sun, but do not account for nucleosynthesis that early in the Sun's life.

Is the distribution of carbon and silicon in the Sun is believed to be uniform, or does it have a radially dependent distribution? Is there be any kind of gravitational settling, i.e. heavier atoms tending to move toward the center as happens in planets?

Since we can only directly measure elemental abundances directly near the surface using spectroscopic techniques, would the radial distribution come from some model or calculation?

**Tags:** the-sun, elemental-abundances
> **Comments:**
> **username_1**: I *believe* what heavier element go to center of core just as it happens with heavier stars.  

---

## 1 answers

### Answer by username_2 on 2016-08-03. Score: 10 | Accepted answer

[A page from the Institute for Advanced Study](http://www.sns.ias.edu/~jnb/SNdata/solarmodels.html) links to data from various modifications to the Standard Solar Model. The newest given there is from [Bahcall1 et al. (2005)](http://arxiv.org/abs/astro-ph/0412440), which I'll use as an example. The authors' calculations depend on data from the Opacity project. Data from two models are available through the IAS link: the [BS05(AGS, OP) model](http://www.sns.ias.edu/~jnb/SNdata/Export/BS2005/bs05_agsop.dat) and the [BS05(OP) model](http://www.sns.ias.edu/~jnb/SNdata/Export/BS2005/bs05op.dat); the difference lies in the main thing you're interested in: heavy element abundances. BS05(AGS, OP) has, for instance, a central2 $^{12}\text{C}$ mass fraction of $7.79\times10^{-6}$, while BS05(OP) has a central $^{12}\text{C}$ mass fraction of $1.05\times10^{-5}$. All of the central data from the major thermodynamic variables (e.g. pressure and temperature), as well as the mass fractions, are well within an order of magnitude in each model.

That said, the general heavy element trend is the same in both models. $^{12}\text{C}$ increase by two to three orders of magnitude from the center. $^3\text{He}$ (rather than the more common $^4\text{He}$, which has a mass fraction given by $Y$) increases by one to two orders of magnitude. $^{14}\text{N}$ actually *decreases* by two orders of magnitude, while $^{16}\text{O}$ remains relatively constant. The model gives no data for silicon.

Other new models agree (though not all), to less than an order of magnitude or so, with the data from Bahcall et al. Graphical representations can be found in e.g. [this paper](http://cos.colorado.edu/~kevinf/PAPERS/solmodel.pdf):

[![enter image description here](https://i.sstatic.net/aQQm7.png)](https://i.sstatic.net/aQQm7.png)

I'm unsure of the reason behind the $^3\text{He}$ spike; that may warrant a follow-up questions. My one guess is that this could be due to its role as an intermediate nucleus in the second step of the [p-p chain](https://en.wikipedia.org/wiki/Proton%E2%80%93proton_chain_reaction). However, the same trends for each element are followed, although the changes in mass fraction are *not* constant at all radii $r$.

As for your question about how the central figures were derived, the answer is that helioseismological measurements and neutrino fluxes are some of the best indicators of composition. This was used as the basis for the BS05(AGS, OP) and BS05(OP) models, as well as, in fact, most variants of the Standard Solar Model.

---

1 This is Bahcall's page, so, naturally, these are some of his papers. However, the results appear to be consistent with the calculations of others.
  
2 Technically, this is from about 0.0016 solar radii, but this distance step is comparatively small.

> **Comments:**
> **username_0**: Wow, thanks for taking the time to put this together. Those plots are *exactly* what I hoped to see - there's so much happening there! Indeed this suggests further questions. Thank you! The footnotes are appreciated as well, I'm pretty sure John Bahcall's papers can be trusted in this context :-).  
> **username_3**: I noticed that there is relatively little overlap between the carbon and nitrogen fraction curves. Might this imply that the CNO cycle is a less common mode of fusion in the Sun?  
> **username_2**: @dualredlaugh The CNO cycle is relatively uncommon in the Sun; it starts becoming dominant at about 1.7$\times$10$^7$ K, a bit higher than the Sun's core temperature. So yes, the p-p chain is far more prevalent than the CNO cycle in Sun-like stars.  
> **username_4**: @dualredlaugh The CNO is energetically unimportant (1%), but *is* responsible for turning almost all the C into N in the core. The N to O (and back to C) bit is much slower.  

---

