Problem on tritons and deuterons

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Discussion Overview

The discussion revolves around the comparative weights of tritons and deuterons versus a helium nucleus and a neutron, exploring the implications of nuclear stability and structure. Participants examine the underlying principles of nuclear mass and stability, referencing various models and hypotheses.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant questions the validity of a book cover suggesting that tritons and deuterons weigh more than a helium nucleus and a neutron, expressing uncertainty about their understanding of the fundamentals.
  • Another participant references a report indicating that the combined mass of a triton and deuteron is approximately 5.030 u, while that of a helium-4 nucleus and neutron is about 5.011 u, supporting the book cover's claim.
  • Some participants discuss the stability of the helium nucleus, suggesting that its even arrangement of protons and neutrons contributes to its stability, while questioning the generality of this principle.
  • One participant challenges the notion that an even number of nucleons always results in stability, citing the instability of Beryllium-8 as an example.
  • Another participant elaborates on the stability of helium-4, proposing that it is due to the attractive forces among its nucleons, while also acknowledging that there may be larger, more stable baryonic structures yet to be identified.
  • A hypothesis is presented regarding Beryllium-8's instability, referencing Linus Pauling's Close-Packed Spheron Model, which posits that stable nuclei beyond mass 4 require specific resonating structures involving tritons or helium-4 clusters.
  • Participants note that no stable isotopes exist for mass 5 or 8, aligning with Pauling's model, and emphasize the historical significance of his contributions to nuclear theory.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between nucleon arrangement and stability, with some supporting the idea of even arrangements leading to stability, while others argue against it. The discussion remains unresolved regarding the broader implications of nuclear stability and the validity of various models.

Contextual Notes

Limitations include the dependence on specific models and hypotheses, as well as the unresolved nature of certain claims regarding nuclear stability and the characteristics of isotopes.

krateesh
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Suppose we have a beam balance capable of measuring even smallest differences in weights.
Now on one side we have a Triton and Deuteron.
And on the other side we have He-nucleus and a neutron

I want to know which will weigh heavier and why?

I saw on a book cover with balance tilting towards the former one thus i concluded that the deuterons and tritons will weigh more but my explanation on that conclusion don't seem to be logical.

Is that book cover right or I have been just fooled and my fumndamentals are just checked?
 
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See table 3.1 in this report: http://book.nc.chalmers.se/KAPITEL/CH03NY3.PDF
The mass of the triton + deuteron ~ 5.030 u, that of helium-4 + neutron ~ 5.011 u. The book cover is correct.
 
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This means helium nucleus is more stable as it do have such even arrangement of both protons and neutrons.
 
krateesh said:
This means helium nucleus is more stable as it do have such even arrangement of both protons and neutrons.

Why would even=stable? Yes, He4 is stable AND seems to be a fundamental building block for heavier elements as He4 is often a decay component. I believe there is a fundamental "structure" to He4 that gives it its stability, though I will admit that the "even" P/N count may provide for this stable structure.
 
2p + 2n is the smallest number of nucleons that can fit into the same ground S-state. At the same time, each of these nucleons feels the attractive force of the nearby other three. That is why He^4 is the stablest nucleus.
Be^8 is not stable because it decays ilnto a pair of these most stable He^4.
 
Meir Achuz said:
2p + 2n is the smallest number of nucleons that can fit into the same ground S-state. At the same time, each of these nucleons feels the attractive force of the nearby other three. That is why He^4 is the stablest nucleus.

I wouldn't categorize that explanations as "why", but it's the current leading theory. "feels attractive force" is a concept with no structure, but I don't disagree. True, He^4 is the most stable known nuclei, but there may still be baryonic nuclear structures "larger" but more stable. One possible candidate would be a baryonic neutrolino, but the current theory gives a huge range of energy values and no composition or structure. Another could be n^4 - no charge, no magnetic moment, very stable and very dense. The later is predicted by W.F. Hagen's second paper on Energiewirbel.

Meir Achuz said:
Be^8 is not stable because it decays ilnto a pair of these most stable He^4.

Hmm.. How about Be^8 is not stable AND it decays into a pair of He^4. Why it is unstable remains unexplained. This decay example does however reinforce one of my first points that He^4 is a building block of larger nuclei.
 
One hypothesis as to why Be-8 is unstable derives from the Close-Packed Spheron Model of Linus Pauling. Here is quote from Pauling: "I assert that nuclei beyond A = 4 are stable only if two or more resonating structures involving hydrogen-3, helium-3, and helium-4 can be written". Dr. Linus Pauling, Research Notebook, #26 . 13 February 1966 :http://osulibrary.oregonstate.edu/specialcollections/rnb/26/rnb26.html

According to this Pauling model there "must" be present a three nucleon cluster, either triton [NPN] or [PNP], rotating against either (1) another three nucleon cluster or (2) a helium-4 cluster (the alpha)for any isotope with A > 4 to be "stable". Hence, Be-8, being composed of two helium-4 rotating clusters [PNPN]~[PNPN] violates this basic "rule of assembly" dynamic and is thus "unstable". Note the same explanation holds for He-5, in fact no mass 5 or 8 isotopes are stable. Now, before anyone starts throwing darts, Linus Pauling was a genius, holds two Nobel Prizes-- and is it not interesting that his model that explains why no stable mass 5 or 8 isotopes exist, published in Science and Proc. National. Acad. Sci. in 1965, has never been falsified.
 
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Rade said:
One hypothesis as to why Be-8 is unstable derives from the Close-Packed Spheron Model of Linus Pauling. Here is quote from Pauling: "I assert that nuclei beyond A = 4 are stable only if two or more resonating structures involving hydrogen-3, helium-3, and helium-4 can be written". Dr. Linus Pauling, Research Notebook, #26 . 13 February 1966 :http://osulibrary.oregonstate.edu/specialcollections/rnb/26/rnb26.html

According to this Pauling model there "must" be present a three nucleon cluster, either triton [NPN] or [PNP], rotating against either (1) another three nucleon cluster or (2) a helium-4 cluster (the alpha)for any isotope with A > 4 to be "stable". Hence, Be-8, being composed of two helium-4 rotating clusters [PNPN]~[PNPN] violates this basic "rule of assembly" dynamic and is thus "unstable". Note the same explanation holds for He-5, in fact no mass 5 or 8 isotopes are stable. Now, before anyone starts throwing darts, Linus Pauling was a genius, holds two Nobel Prizes-- and is it not interesting that his model that explains why no stable mass 5 or 8 isotopes exist, published in Science and Proc. National. Acad. Sci. in 1965, has never been falsified.

Great link, thanks!
 

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