Nuclear Fission of Uranium-235

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Discussion Overview

The discussion revolves around the nuclear fission of uranium-235, specifically focusing on the behavior of uranium-236 produced during the fission process. Participants explore the stability of uranium-236, its decay modes, and the conditions under which it may or may not fission. The scope includes theoretical aspects of nuclear physics and the implications of nuclear stability.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant claims that uranium-235 fissions 82% of the time upon neutron absorption, briefly forming excited uranium-236 before splitting, while 18% of the time it produces uranium-236 without fission, raising questions about the stability of uranium-236.
  • Another participant discusses the instability of larger atomic nuclei, noting that uranium is on the verge of instability due to the balance between the strong force and Coulomb repulsion, suggesting that even mass numbers tend to be stable while odd ones are not.
  • A different participant explains that excited uranium-236 is likely to fission, but if it emits a photon, it transitions to a ground state that is unlikely to fission, indicating that this transition essentially prevents fission from occurring.
  • Another contribution elaborates on the concept of nuclear states, explaining that ground states are more stable than excited states and that uranium-236's ground state is not stable, which could lead to decay into other nuclei and particles.
  • Gamma decay is mentioned as a process where excited states emit high-energy photons to release excess energy, drawing a parallel to electron de-excitation in atoms.

Areas of Agreement / Disagreement

Participants express varying views on the stability of uranium-236 and the conditions under which it may fission or decay. There is no consensus on the implications of these processes, and the discussion remains unresolved regarding the specifics of uranium-236's behavior.

Contextual Notes

Participants reference the concepts of nuclear stability, excited states, and decay modes, but there are limitations in the assumptions made about the conditions under which these processes occur. The discussion does not resolve the complexities involved in the behavior of uranium-236.

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TL;DR
Nuclear Fission of Uranium-235
I'm learning about nuclear fission for fun, well based on my research, 82% of the time that uranium-235 absorbs a neutron it will fission, the uranium-235 will briefly turn into an excited uranium-236 and after that, it will split, the other 18% of the time it will just emit radiation and produce uranium-236, that one being radioactive waste, but isn't the uranium-236 unstable to the point where it will split in the same way? What's the difference between the two situations?

I may have said something wrong, correct me please, thanks.
 
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Atom nuclei for larger atomic numbers become unstable due to short range of attractive strong force and larger repulsive Coulomb force. Uranium is on the verge. A neutron difference in nuclei dominates the future of the nuclei. In general even mass numbers make it stable and the odd one make it unstable.
 
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The U-236 is produced in an excited state which is likely to fission. If it emits a photon then it goes to its ground state, which is unlikely to fission. So unlikely that it's essentially not happening at all. U-236 is still radioactive but it has a long half life and the dominant decay mode is an alpha decay.
 
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Nuclei with a certain number of protons (Z) and neutrons (N = A-Z) can exists in different states. The ground state is the state with lowest energy and correspond to the configuration of those Z protons and N neutrons which has the highest amount of binding energy (which is equivalent to lowest total mass). But there are many ways one can re-arrange those protons and neutrons - those states are called excited states and have lower binding energy than the ground state (which is equivalent to higher total mass).

Ground states does not have to be stable and can thus decay to other nuclei and particles, but they are waaaay more stable than excited states. This is the case for U-236, its ground state is not stable, which was mentonied in the post before mine here.

Gamma decay is when the protons and neutrons rearrange in an excited state and emitts high energy photons to get rid of excess energy. Quite similar to de-excitation of eletrons in an atom which you might be familiar with.
 
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