Abstract

A proton beam with a velocity of the order of 10^9 cm/s is generated to interact with a charge neutral hydrogen-boron medium such as H3B. The created charged particles are confined by magnetic fields. This concept was the basis for a novel non-thermal fusion reactor, published recently in Laser and Particle Beams [1]. The fusion is initiated by protons followed by a process of chain reactions in a neutral medium density of the order of 10^19 cm-3, heated by the pB11 fusion created alphas up to a temperature of about one electron volt. In this system, the radiation losses by bremsstrahlung are negligible and the plasma thermal pressure is low. The ionization of the gaseous medium is caused by the alpha elastic nuclear collisions with the hydrogen atoms and their thermal heating and it is less than 10^-4. An external electric field is applied to avoid the energy losses of the protons particles by friction, due to their interaction with the electrons of the medium, to keep the proton-boron fusion at the maximum cross section of about 600 keV at the center of mass frame of reference. The alphas created in the pB11 fusion undergo nuclear elastic collisions with the hydrogen protons of the medium and causing a pB11 chain reaction. In this paper the equation of motion of these proton and alphas are solved numerically for the one-dimensional (1D) case, and their possible solutions are analyzed and discussed. Specifically, it is shown how the electric field can mitigate the stopping power for the proton11-proton nuclear fusion. Our results show that starting from a bunch of 1013 protons in our volume, an alpha number of particles of 6×10^16 was accepted after a 5ms cycle of applying our specially designed electric field. Consequently, the medium temperature was raised to 1.3 eV. Although the aim of this paper is to present a new concept by addressing only the main physical processes and not to present a complete engineering design for a power plant, our numerical solution is novel and promises a viable proton-boron11 fusion reactor for clean energy creation.

Highlights

  • Two different distinctive schemes for solving the energy problem with fusion have been investigated in the past 60 years: (1) Magnetic confinement fusion (MCF) based on high intensity magnetic fields confining low-density (∼1014 cm−3) and high temperatures (∼10 keV) plasmas for long or practically continuous times (2)

  • In a recent paper [1] a novel concept for a nuclear fusion reactor has been proposed for proton-boron11 yielding 3 alphas, p +11 B → 3α + 8.9MeV. In this novel reactor [1] the fusion events are initiated by protons accelerated by a high power laser followed by a process of chain reactions in a medium. This medium (e.g., H3B) is a charge-neutral gas with a density of the order of 1019 cm−3 that is heated to a maximum one electronvolt, so that the radiation level and the plasma thermal pressure are very low

  • Power Problem we describe our chain reaction and the alpha energy losses due to their interaction with the electrons

Read more

Summary

INTRODUCTION

Two different distinctive schemes for solving the energy problem with fusion have been investigated in the past 60 years: (1) Magnetic confinement fusion (MCF) based on high intensity magnetic fields (several Teslas) confining low-density (∼1014 cm−3) and high temperatures (∼10 keV) plasmas for long or practically continuous times (2). We use an external electric field acting on the charged particles in the medium with densities of the order of 1019 cm−3 and temperature of the order 1 eV or less These electromagnetic field prolong the chain reaction process in a reasonable volume [1] (∼104 cm3) by overcoming the Bethe-Bloch energy loss [12] of the alphas and protons due to their collisions with the bound electrons in our neutral gas, dTA dx. Calculating the protons (at 0.6 MeV) and alphas (at 3 MeV) mean free path from the stopping power of our medium yields 10 and 25 cm, respectively This short distance (which may be shortened further by increasing the medium density) enables us to disregard the scattering angle and consider our schema as 1D.

DISCUSSION AND CONCLUSION
Findings
DATA AVAILABILITY STATEMENT
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call