Chemical Elements produced inside the Sun

In summary, the conversation discusses the possibility of the nuclear processes inside the Sun producing heavier elements such as iron and uranium. The participants agree that the Sun is not capable of producing these elements due to its size and energy limitations. The conversation also touches on the concept of elements already existing in the Sun's initial state and the process of nucleosynthesis occurring in more massive stars. Finally, there is a brief discussion about the laws of thermodynamics and the probability of heavier elements being created in the Sun.
  • #36
phyzguy said:
The proton-proton cycle fuses protons to deuterium. D + D fuses to He3 + n or T + p with equal probability, and of course D + T gives He3 + n. So, given the size of the sun, many free neutrons are produced.
D+D is extremely rare. For every deuterium nucleus there are ~1017 protons around for p+D -> He-3 + photon. It does happen, so some tritium is produced. But then you have the same problem again: Deuterium is extremely rare. p+T -> He-4 + photon is much more likely than D+T -> He-4 + n. I guess a few neutrons are produced via this reaction path, but the total number must be really small.
Vanadium 50 said:
That's not as big a number as it looks. Uranium requires 237 nucleon additions. What does that mean for the probability of each nucleus to glom on another nucleon? Is it 0.1%? 1%? 10%? No - it has to be 71%, otherwise you don't get all the way to uranium.
You don't have to start with hydrogen. The Sun contains all long-living isotopes already from its formation, for most elements you just have to add one more neutron and wait for a decay, or just wait for a decay.
Vanadium 50 said:
That said, I believe every (natural) element is present in the sun, but for another reason: uranium fission. The tiny bit of primordial U-235 in the sun is exposed to neutrons and will fission.
The fraction of induced fission of U-235 should be tiny, but there is spontaneous fission. I said this many posts ago already.
DaTario said:
but in order to be complete, if those heavy elements were not present, would the natural ascending (starting basically from H) processes of nucleosynthesis provide all the elements?
If the Sun would have started with hydrogen exclusively it wouldn't contain uranium by now. Probably not even iron.
 
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  • #37
DaTario said:
So, due to the preexising Uraniun inside the Sun, which was there even before the star is born, other elements are then produced. This seems to provide a valid answer to the question in the OP, but in order to be complete, if those heavy elements were not present, would the natural ascending (starting basically from H) processes of nucleosynthesis provide all the elements?
The short answer is no. From a fusion point of view Iron is the end of the line, to continue fusion requires energy to be input, which is why the heavier elements are formed by supernovae. Because the heavier elements are found on Earth it has been known for quite some time that the sun is at least a second generation star, but it is probably 3rd or even fourth generation.
 
  • #38
John Collis said:
to continue fusion requires energy to be input
There is nothing fundamentally problematic with endothermic reactions.
To study if the reaction happens you need a quantitative statement - how much energy is necessary. Too much for fusion of iron to heavier elements, but the same is true much earlier in the Sun. There is nothing special about iron in the current Sun.
 
  • #39
jim mcnamara said:
@phyzguy

I think we have partial verification of the claim "all elements". Could you please provide us with a citation that helps to clear this up fully? Thank you kindly...
Well, I don't have a peer-reviewed document, but below is a set of lecture notes:

http://www.uio.no/studier/emner/matnat/astro/AST1100/h06/undervisningsmateriale/lecture-7.pdf

In addition to the D+D source of neutrons I mentioned earlier, this source also talks about several other sources of neutrons in the CNO cycle, which probably have higher reaction rates in the sun. From the above lecture notes:

"The r and s processes There is an exception to this temperature rule if there is a source of neutrons present as neutrons do not feel the Coulomb force. It is possible to distinguish material synthesized in a neutron rich environment from that synthesized in a neutron poor one. s-process (‘s’ for slow) elements are those formed where β-decay is expected to occur before a neutron is absorbed, while r-process 6 (‘r’ for rapid) elements are those formed where new neutrons can be absorbed readily. Sources of neutrons are various, for examples such chains as
He4 + C13 → O16 + n
O16 + 16O → S31 + n

Free neutrons produced in this manner are a way of forming elements beyond the iron peak in binding energy. In ordinary circumstances in stellar cores it is the s-processes that dominate, in extreme situations such as in supernova r-process nucleosynthesis can occur."

I'm not claiming the above reactions are common, or that the free neutrons produced are abundant, but we are talking one atom out of the ~10^59 nucleons in the solar core.
 
  • #40
And what are the expected lifetimes of these high-neutron isotopes? Especially compared to the time the nucleus needs to wait to capture another, and another, and another neutron? Getting from lead/bismuth to uranium is hard, and venturing into the realm of superheavies is not very probable even in environment with far higher neutron fluxes, like supernovae. Intermediates needed to clear the gaps in the nuclide chart have too short half-lives. Though it would require checking the numbers to tell how improbable it is for even one in 1059 nucleons throughout all 10–12 billion years of Sun's existence.
 
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  • #41
I was wrong about solar mass stars having convective cores - they're radiative. But this doesn't negate the fact that temperatures in the cores of solar mass stars aren't high enough to produce elements beyond carbon, oxygen, and nitrogen, and the C-N-O cycle doesn't occur in solar mass stars. The s-process and r-process elements are produced exclusively in stars of 8 solar masses and greater.
 
  • #42
alantheastronomer said:
...The s-process and r-process elements are produced exclusively in stars of 8 solar masses and greater.

This paper says most of the s-process elements come from stars with mass 1Θ to 3Θ.
alantheastronomer said:
... But this doesn't negate the fact that temperatures in the cores of solar mass stars aren't high enough to produce elements beyond carbon, oxygen, and nitrogen, and the C-N-O cycle doesn't occur in solar mass stars. ...

They are asymptotic giant branch stars. The temperatures are far above what is needed for CNO cycle. They have helium burning in explosive flashes. The s-process elements reach the surface in a series of 3rd dredge ups.

R-coronae Borealis has a mass less than the sun. It lacks hydrogen and there is a class of objects call R-coronae borealis variables most of which also have a hydrogen shortage. The variability comes from puffs of carbon soot blowing out into a planetary nebula.

Sakurai's object is worth reading about too. It has 0.6 solar mass. It was observed coughing up s-process elements in 1996.

The Sun has some CNO cycling according to wikipedia:
pp-chain reaction starts at temperatures around 4×106 K, making it the dominant energy source in smaller stars. A self-maintaining CNO chain starts at approximately 15×106 K, but its energy output rises much more rapidly with increasing temperatures. At approximately 17×106 K, the CNO cycle starts becoming the dominant source of energy. The Sun has a core temperature of around 15.7×106 K, and only 1.7% of 4
He nuclei produced in the Sun are born in the CNO cycle.
 
  • #43
The paper states that the s-process nuclei are produced in stars of 1.5-3 solar masses not 1-3 solar masses, but your point is well taken. Also, Ratman's comments in post #40 are entirely relevant!
 
  • #44
Sun is not now hot enough to produce carbon and oxygen out of helium by triple alpha process.
However, Sun is hot enough to interconvert preexisting carbon, nitrogen and oxygen by CNO cycle.
Which other preexisting elements can Sun convert?
 
  • #45
It seems, given what was said here so far, that, in a realistic model of the Sun, it may have (or have had at some time) the complete set of chemical elements inside, as it has come from a supernovae explosion. It seems that all these elements, specially the heavier ones, are unlikely to survive for long time.
I understand that, once all the heavier ones have been broken in small pieces, and due to the Sun's thermodynamic condition, the reposition of the complete set of chemical elements turns out to be impossible. Would this description be a reasonable synthesis of all that we had here?
 
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  • #46
DaTario said:
It seems, given what was said here so far, that, in a realistic model of the Sun, it may have (or have had at some time) the complete set of chemical elements inside, as it has come from a supernovae explosion. It seems that all these elements, specially the heavier ones, are unlikely to survive for long time.
I understand that, once all the heavier ones have been broken in small pieces,
How much fission does actually happen in Sun?
 
  • #47
DaTario said:
It seems, given what was said here so far, that, in a realistic model of the Sun, it may have (or have had at some time) the complete set of chemical elements inside, as it has come from a supernovae explosion. It seems that all these elements, specially the heavier ones, are unlikely to survive for long time.
I understand that, once all the heavier ones have been broken in small pieces, and due to the Sun's thermodynamic condition, the reposition of the complete set of chemical elements turns out to be impossible. Would this description be a reasonable synthesis of all that we had here?
The sun will keep having some uranium (and its decay products) for hundreds of billions of years, much longer than its lifetime as star.
 
  • #48
mfb said:
The sun will keep having some uranium (and its decay products) for hundreds of billions of years,
100 Gyr is 22 half-lives for U-238.
 
  • #49
snorkack said:
100 Gyr is 22 half-lives for U-238.

When we speak of half-life we mean the atom left alone, don´t we?
Inside the Sun the mean durations of practically every chemical element tend to be far shorter than these estimates (half-lives), aren´t they?
 
  • #50
DaTario said:
When we speak of half-life we mean the atom left alone, don´t we?
Inside the Sun the mean durations of practically every chemical element tend to be far shorter than these estimates (half-lives), aren´t they?
Every RADIOACTIVE element...the abundances of these elements are far too small for chain reactions to change their half-lives appreciably!
 
  • #51
snorkack said:
100 Gyr is 22 half-lives for U-238.
It means the number of atoms will drop by a factor of 5.5 million. The number of uranium atoms in the Sun will go down from about 1042.5 to 1036.
We expect the last atom to decay after about 140 half lives, or 630 billion years, neglecting that the Sun constantly gets new uranium atoms from the outside. Atoms are small, there are many of them.
DaTario said:
When we speak of half-life we mean the atom left alone, don´t we?
Inside the Sun the mean durations of practically every chemical element tend to be far shorter than these estimates (half-lives), aren´t they?
The environment in the Sun doesn't change radioactive decays in any relevant way.
 
  • #52
Sun produces a lot of D.
Sun does not contain much of it, because it readily reacts. A major fate of d is
d+p→3He+γ
despite being an electromagnetic process.
This keeps the abundance of d low, so processes like
d+d→3He+n
have a low branching fraction
p is not the only common nucleus in Sun. But reaction
d+α→6Li+γ
is also electromagnetic, and faces a high Coulomb barrier.
How about reactions like
d+12C→13C+n?
It is a strong process, not electromagnetic.
And the proton does not need to get across the Coulomb barrier...
Is this a common fate for metals in Sun?
 
  • #53
You mean d+12C→13C+p?
The Coulomb barrier is still there - the nuclei have to get close together to make the neutron transfer possible.
Didn't check the energy balance of the reaction. 13C is part of the CNO cycle. This reaction, if possible, mixes the two fusion chains.
 
  • #54
phyzguy said:
...So, given the size of the sun, many free neutrons are produced.
mfb said:
...The environment in the Sun doesn't change radioactive decays in any relevant way.

These two statements look contradictory. My understanding was that uranium 235 fissions when it is hit with a neutron. Uranium 238 can fission with fast neutrons and becomes plutonium 239 (via Np239) when exposed to slow neutrons. Plutonium 239 has a much shorter half life than U238. Pu239 will alpha decay to U235 or fission when exposed to neutrons.

"Fission reaction" is not the same as "radioactive decay". DaTario actually wrote "mean durations of chemical elements" so reactions should count too.
 
  • #55
stefan r said:
These two statements look contradictory. My understanding was that uranium 235 fissions when it is hit with a neutron. Uranium 238 can fission with fast neutrons and becomes plutonium 239 (via Np239) when exposed to slow neutrons. Plutonium 239 has a much shorter half life than U238. Pu239 will alpha decay to U235 or fission when exposed to neutrons.

"Fission reaction" is not the same as "radioactive decay". DaTario actually wrote "mean durations of chemical elements" so reactions should count too.
Different posters, different beliefs as to facts.
Sun is big so Sun produces a large number of free neutrons.
However, these neutrons are a small fractions of all nuclei present in Sun, being so big. Induced fission is a small effect in the Sun.
The major free neutron producing reactions for s-process are
13C+α→16O+n
22Ne+α→25Mg+n
These reactions have a high Coulomb barrier, and Sun is not hot enough for them.
The likely reaction is
d+d→3He+n
but this is a minor side reaction because of competing reaction
d+p→3He+γ
Therefore the free neutron flux in Sun is modest at present.
How is the radial distribution of that neutron flux?
 
  • #56
stefan r said:
"Fission reaction" is not the same as "radioactive decay".
Exactly.
Not that the neutrons would matter - in absolute numbers there are a lot of them, but they get absorbed by other elements quickly.
 
  • #57
mfb said:
Not that the neutrons would matter - in absolute numbers there are a lot of them, but they get absorbed by other elements quickly.
Mainly protium.
 
  • #58
There aren't many free neutrons in the solar core - d+d -> He-4 NOT He-3 + n, and the half-life of free neutrons is only fifteen minutes!
 
  • #59
d + d -> He-4 + photon is a very rare reaction as it needs the electromagnetic interaction. d + d -> He-3 + n and d + d -> T + p are much more common (about 50% each).
alantheastronomer said:
and the half-life of free neutrons is only fifteen minutes!
Doesn't matter, neutrons in matter are nearly always caught (~microseconds, probably even less in the Sun) before they decay. You have to carefully keep them away from matter to observe their decays.
 
  • #60
alantheastronomer said:
I was wrong about solar mass stars having convective cores - they're radiative. But this doesn't negate the fact that temperatures in the cores of solar mass stars aren't high enough to produce elements beyond carbon, oxygen, and nitrogen, and the C-N-O cycle doesn't occur in solar mass stars. The s-process and r-process elements are produced exclusively in stars of 8 solar masses and greater.

New information. The R-process seems to be an exclusive result of a kilonova, the merger of two neutron stars. We could discuss the latest on the maximum mass of a neutron star, but the kilonova, will be less than about 3 solar masses total. A kilonova was recently detected by LIGO then by lots of telescopes all across the electromagnetic spectrum. https://www.vox.com/science-and-hea...igo-gravitational-waves-neutron-star-kilonova The result was almost purely R-process elements, pretty much matching not only the expected abundances, but theoretical calculations. The result is that more than 90% and probably all of the R-process elements come from kilonovas.

I guess you could say that each of the (two) stars involved were originally high enough mass (but not too high) to go supernova and leave a neutron star. Then the neutron stars have to spiral in for the kilonova--there are some pairs out there which won't merge for tens of billions of years. So kilonovas are pretty rare, and galaxies without one in their history are missing R-process elements. Oh, and you get a short gamma-ray burst. Lots of newly settled science from that one event.

To relate this to the original post, almost every R-process atom in the sun came from a kilonova.
 
  • #61
eachus said:
The R-process seems to be an exclusive result of a kilonova, the merger of two neutron stars.
Yes it's true that the R-process elements observed in this event closely matched the predicted ratios - except for the higher mass end. Since we don't yet have a working model of a supernova explosion, it's impossible to estimate the R-process yields of such an event. It's worth noting that the frequency of supernova explosions is approximately one to two per century per galaxy while, as you have noted, the timescale for the merger of binary neutron stars is at least hundreds of thousands of years.
 
  • #62
alantheastronomer said:
Yes it's true that the R-process elements observed in this event closely matched the predicted ratios - except for the higher mass end. Since we don't yet have a working model of a supernova explosion, it's impossible to estimate the R-process yields of such an event. It's worth noting that the frequency of supernova explosions is approximately one to two per century per galaxy while, as you have noted, the timescale for the merger of binary neutron stars is at least hundreds of thousands of years.

Good point. If some supernovas form degenerate cores even seconds before the explosion, and don't form a white dwarf, neutron star or black hole, they will probably form, and release into the interstellar medium some R-process elements. I thought I left enough wiggle room for that. However, I suspect that most of these elements if formed will get locked away inside whatever stellar remnant is formed. Looking at the spectra of white dwarfs would be the best way to look for this. (But white dwarf production is probably the signature of the mildest supernovas.) The data for white dwarf spectra that I have looked at pretty much has iron and nickel as the heaviest elements.

Hmm. That seems to say that at some point, in heavy stars core burning migrates outward. Think of Hydrogen or Helium burning when the core is nearly depleted. The burning would migrate to where the fuel was, which can happen much faster than atoms can move in the core. When burning produces iron the burning is still moving outward. If the core then cools, by neutrino emission if no other way, it will collapse and boom! The signature of iron production outside the core, would be iron in the outer layers of recently produced white dwarfs. I'm retired, and modelling that looks like a big job with a supercomputer needed for the calculations. So if anyone wants to take that idea and run with it? Feel free.
 
  • #63
eachus said:
The signature of iron production outside the core, would be iron in the outer layers of recently produced white dwarfs.
You seem to be confusing white dwarfs with neutron stars. Neutron stars are the end products of supernova explosions, while white dwarfs are the cores of lower mass stars as they turn into red giant stars and ultimately planetary nebulae. To find a more thorough description look up "Stellar Evolution" and "Supernovae" in Wikipedia.
eachus said:
I suspect that most of these elements if formed will get locked away inside whatever stellar remnant is formed.
There is still nucleosynthesis going on in the layers of material outside the core, and r-process elements could conceivably be produced there during the explosion, if we only knew what that mechanism was.
 
  • #64
I find it curious that the emissions of supernovae and similar contain so much heavy elements.
Obviously they do, otherwise rocky planets like Earth could never form.
Intuitively one would think that most of the heavy elements produced end up within the remnant of a core.
Typically that is a white dwarf.or a neutron star.
 
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  • #65
alantheastronomer said:
You seem to be confusing white dwarfs with neutron stars. Neutron stars are the end products of supernova explosions, while white dwarfs are the cores of lower mass stars as they turn into red giant stars and ultimately planetary nebulae.

I'm not confused. I'm trying to show that even at their hottest, white dwarfs do not produce significant amounts of iron. In the hottest white dwarfs helium burns to carbon and oxygen. Forming higher weight atoms by adding additional alpha particles doesn't occur, due to the higher and higher temperatures required. However, it is possible that higher weight atoms (up to Ni56 (which decays to Fe56.) could be produced by the s-process but the lack of heavier metals, especially iron, says that there are not enough neutrons floating around to produce them. (Some white dwarfs do have traces of elements up to silicon, but it is no clear if they are collected from nearby supernova or interstellar gas.
 
  • #66
eachus said:
I'm not confused. I'm trying to show that even at their hottest, white dwarfs do not produce significant amounts of iron.
Oh, I see what you're saying! Sorry, never mind.
eachus said:
I suspect that most of these elements if formed will get locked away inside whatever stellar remnant is formed.
rootone said:
Intuitively one would think that most of the heavy elements produced end up within the remnant of a core.
In high mass stars that have formed iron cores that are ready to collapse, there is still shell burning of elements leading up to iron outside of the core. It is the mixing of these layers, and the rapid expulsion of neutrons from the surface of the newly formed neutron star by whatever mechanism that causes the supernova explosion, that presumably produces the rest of the heavier elements.
 
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