Distribution of released energy in nuclear fusion

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Discussion Overview

The discussion revolves around the distribution of energy released in nuclear fusion reactions, particularly focusing on whether this energy manifests solely as kinetic energy of the products, the possibility of excited states, and the emission of gamma photons. The scope includes theoretical considerations of fusion reactions at low energies, up to ± 30 MeV.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants propose that the energy released in fusion reactions typically manifests as kinetic energy of the products, although gamma rays can be emitted in rare cases.
  • There is a suggestion that if only one nuclide is produced, the total energy cannot be entirely transferred to that product due to energy-momentum conservation principles.
  • One participant requests clarification on the violation of energy-momentum conservation in the context of fusion reactions producing a single nuclide.
  • A later reply elaborates on the conservation of energy and mass in fusion reactions, explaining that if the final product is at rest, the kinetic energy of the reactants must account for the energy balance, leading to the conclusion that negative kinetic energy is not possible.
  • Another participant mentions the CNO cycle, noting the emission of gamma rays and positrons, which contribute to the total energy output in fusion processes.

Areas of Agreement / Disagreement

Participants express differing views on the mechanisms of energy distribution in fusion reactions, with some agreeing on the role of kinetic energy while others raise questions about the implications of energy-momentum conservation. The discussion remains unresolved regarding the specifics of energy distribution and the conditions under which gamma emissions occur.

Contextual Notes

The discussion includes assumptions about the nature of fusion reactions and the conditions under which energy is released. There are unresolved aspects regarding the treatment of excited states and the specific mechanisms of energy transfer in different fusion pathways.

Toreno
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Hi,

On Wikipedia (here), we can find that in following channels of nuclear fusion reactions:
H-2 + H-3 -> He-4 (3.5 MeV) + n (14.1 Mev)
H-2 + H-2 -> H-3 (1.01 MeV) + H-1 (3.02 MeV)
H-2 + H-2 -> He-3 (0.82 MeV) + n (2.45 MeV)
H-2 + He-3 -> He-4 (3.6 MeV) + H-1 (14.7 MeV)
The released energy is always distributed between products.
But I have a few questions regarding above and other reaction channels:

1) Does this energy always manifests as kinetic energy of products?
2) If no, does the product nuclide can be created in excited state (and consume some of kinetic energy)?
3) or may a gamma photon be emitted consuming some the energy?
4) and finally, if only one nuclide is produced (e.g. He-4), does whole energy is transferred to that product?

Oh, I am talking about reactions in low energies, up to ± 30 MeV.

Many Thanks,
Toreno
 
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Toreno said:
1) Does this energy always manifests as kinetic energy of products?
Most of the time. All those reactions can happen with the emission of gamma rays (directly), but that is a rare process. I don't think there are nuclear excitations that don't decay via proton or neutron emission (which effectively looks like a different reaction then).
Toreno said:
4) and finally, if only one nuclide is produced (e.g. He-4), does whole energy is transferred to that product?
That would violate energy-momentum conservation.
 
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Hi,

Thank you for fast response.
Could you please expand a little more that energy-momentum violation?

Thanks,
Toreno
 
Toreno said:
Could you please expand a little more that energy-momentum violation?

Suppose for the sake of discussion that the fusion reaction X + Y --> 4He exists, and that there are no other products (e.g. gammas).

Recall that in a fusion reaction that releases energy, the sum of the masses of the reactants must be greater than the sum of the masses of the products. In this case, we must have

m(X) + m(Y) > m(4He).

Consider this reaction in the reference frame in which the final 4He is at rest. That is, its kinetic energy K(4He) = 0. The total energy must be conserved. Therefore we must have

m(X)c2 + K(X) + m(Y)c2 + K(Y) = m(4He)c2

The previous condition then implies that either K(X) or K(Y) or both must be negative. But kinetic energy can't be negative!
 
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Ok, I got this now. Thank you for. Thank you for explanation!
 
The CNO cycle emits 3 gamma rays in each turn of the cycle, and 2 positrons, which, upon annihilation, generate 4 additional gamma rays, bringing the total to 7.
 

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