soizndxzp3239 said:
Yes, I wasn't thinking of that. All that potential energy did we give to the proton in the first place by removing the electron.
If you confine the experiment in vacuum with no photons, why will there still be charge leakage?
Of course one would accelerate charges in a vacuum, otherwise the charges would collide with gas atoms and lose energy. There is no perfect insulator, and there is some high voltage potential with which one is accelerating protons (or some positively charge nuclei).
But if you put many of these devices in a line the protons will have enough energy to break the coulomb barrier and few of them will be scattered due to quantum dynamics, right?
The purely static potential is problematic. One has to move the electrons to the negatively charged target. If one is thinking of cascading accelerating potentials, that's not really how one would do it for a low (few kV) potential. The static (relatively constant) potential is just a DC potential. The scattering occurs because the target is comprised of atoms, and the projectile particles travel through the electrons surrounding the atoms, which are ionized, and scatter off the nuclei. The coulomb interaction range is much greater than the range of nuclear interactions.
If there is a nuclear reaction there will always be thermal energy released, right? Ex. Translation, vibration or angular momentum of the products. The energy needed to ionize the hydrogen is far less than the energy received from the fusion, the magnitude of 10^3. I would guess that a Stirling engine connected to a generator has a efficiency of more than 0.001?
If there is a nuclear reaction, there will be some energy released, e.g., kinetic (thermal) energy of the products, or in the case of p + d, the kinetic energy of an He
3 nucleus + a gamma ray, and the gamma ray would then scatter off atomic electrons (Compton effect) or be absorbed (photoelectric effect). That energy heats the solid target, which could in theory be used to heat a working fluid.
The 13.6 ev ionization energy of hydrogen is certainly much less than the MeV levels of energy liberated in fusion reactions, but one has to consider the reaction rate for fusion vs scattering, which is a function of the cross-section of the reaction, and densities of the target and projectile particles. If one obtains one fusion reaction for every 100,000 projectile particles, then there isn't much net energy produced, especially if one uses a thermodynamic cycle with a conversion efficiency less than 30-40%.
I haven't looked at the p+d or p+t cross-sections for fusion reactions, so I really don't know how low they are. Most fusion systems are considering d+d or d+t fusion, and some p + B
11.