CNO fusion using particle accelerator?

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Discussion Overview

The discussion revolves around the feasibility of achieving the CNO fusion cycle in a laboratory setting using a particle accelerator. Participants explore the theoretical underpinnings of the CNO cycle, the challenges of overcoming Coulomb repulsion, and the potential for energy capture from gamma rays produced during the process.

Discussion Character

  • Exploratory, Technical explanation, Debate/contested

Main Points Raised

  • One participant describes the CNO cycle as a catalytic fusion reaction that converts protons into helium-4, releasing energy primarily as gamma rays.
  • Another participant argues that while high-energy nuclei can be fired at a target, the majority will not fuse due to Coulomb scattering, leading to insufficient fusion energy compared to the energy required for acceleration.
  • A suggestion is made to insert the target into the accelerator ring to recycle beam particles that do not collide with target nuclei, potentially increasing collision chances.
  • Another participant clarifies that even with this approach, particles still collide but may not do so head-on, resulting in deflections or energy loss through interactions with electrons.

Areas of Agreement / Disagreement

Participants express differing views on the practicality of using particle accelerators for CNO fusion, with some proposing innovative ideas while others highlight fundamental challenges, indicating that the discussion remains unresolved.

Contextual Notes

Participants note limitations related to the efficiency of fusion energy production versus energy input, as well as the complexities of particle interactions within the accelerator environment.

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The CNO cycle (see https://en.wikipedia.org/wiki/CNO_cycle) is a catalytic fusion reaction that produces energy in stars larger than the sun. It converts four protons into a helium-4 nucleus using a cycle of carbon, nitrogen and oxygen isotopes as catalysts and releases 26.7 MeV of energy mostly in the form of gamma rays.

Could one make this cycle work in the laboratory by bombarding a high-density target made of these isotopes with protons accelerated in a particle accelerator?

If a carbon nucleus has a radius of about ##2.7\times10^{-15}## m then one would require protons to be accelerated to about ##3.2## MeV in order to overcome the Coulomb repulsion. I guess this can easily be achieved. If the energy of the gamma rays was captured perhaps one could produce fusion energy by this method?
 
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Many people have thought about trying to produce fusion with particle accelerators. Suppose I fire high-energy nuclei at a target (say I fire deuterium nuclei at a deuterium target). A very few of the nuclei will hit a target nucleus "head-on", overcome the Coulomb barrier, and fuse. The vast majority of the incoming nuclei, however, will lose their energy through Coulomb scattering off the nuclei and electrons in the target. The amount of fusion energy produced in this way is far less than the energy needed to accelerate the incoming nuclei. It just doesn't work.
 
Could one insert the target into the accelerator ring so that any beam particles that don't collide with target nuclei are collected and sent round the accelerator again until they do collide?
 
They still collide, they just don't collide with a nucleus head on. They collide with a nucleus with a non-zero impact parameter and are deflected or they collide with electrons and lose energy.
 

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