Towards p-11B medium configurations with high Pfus/PBrems ratios

Aneutronic p-11B nuclear fusion is promising for clean energy production, as it produces three (3) alpha particles with 8.7 MeV total energy. However, the main difficulty for p-11B fusion ignition (Q = Pfus/PBrems≥ 1) concerns the nuclear cross section and thus, reactivity efficiency at higher than...

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Main Authors: C. Daponta, S. Moustaizis, S. Eliezer, Z. Henis, P. Lalousis, N. Nissim, Y. Schweitzer
Format: Article
Language:English
Published: Frontiers Media S.A. 2024-11-01
Series:Frontiers in Physics
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Online Access:https://www.frontiersin.org/articles/10.3389/fphy.2024.1425963/full
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author C. Daponta
S. Moustaizis
S. Eliezer
Z. Henis
P. Lalousis
N. Nissim
Y. Schweitzer
author_facet C. Daponta
S. Moustaizis
S. Eliezer
Z. Henis
P. Lalousis
N. Nissim
Y. Schweitzer
author_sort C. Daponta
collection DOAJ
description Aneutronic p-11B nuclear fusion is promising for clean energy production, as it produces three (3) alpha particles with 8.7 MeV total energy. However, the main difficulty for p-11B fusion ignition (Q = Pfus/PBrems≥ 1) concerns the nuclear cross section and thus, reactivity efficiency at higher than 200 keV medium temperatures. To overcome this difficulty, the present work emphasizes on the numerical investigation of medium schemes (configurations) with enhanced reactivity. The configurations refer to the addition of energetic protons in a low-density 11boron or proton–11boron medium (n = 1020 m−3), with (np/nB) > 1 for Bremsstrahlung losses optimization and initial temperature in the range of 1 keV ≤ Tin≤ 400 keV. A self-consistent multi-fluid global particle and energy balance code, including collisions between all medium species (p, 11B, e, α), is used for the description of the temporal evolution of all fusion medium physical parameters and the evaluation of the optimum initial conditions for the obtainment of Q ≥ 1. The numerical simulation results show that the coupling between the 200 keV < Ep,0≤ 750 keV energetic protons and the 1 keV ≤ Tin≤ 400 keV initial fusion medium leads to ignition, 1 ≤ Q < 1.4, below Tin= 100 keV. In all the presented initial medium temperature cases, and especially, the lower (<) than 100 keV, the ignition condition (Pfus/PBrems) > 1 arises, as a consequence of the chain reactions and the related avalanche alpha heating effect.
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spelling doaj-art-4b89338087a1487aaa3f1c893e2b9eca2024-11-15T04:52:45ZengFrontiers Media S.A.Frontiers in Physics2296-424X2024-11-011210.3389/fphy.2024.14259631425963Towards p-11B medium configurations with high Pfus/PBrems ratiosC. Daponta0S. Moustaizis1S. Eliezer2Z. Henis3P. Lalousis4N. Nissim5Y. Schweitzer6Lab of Matter Structure and Laser Physics, Technical University of Crete, Chania, Crete, GreeceLab of Matter Structure and Laser Physics, Technical University of Crete, Chania, Crete, GreeceApplied Physics Department, Soreq Nuclear Research Center, Yavne, IsraelApplied Physics Department, Soreq Nuclear Research Center, Yavne, IsraelInstitute of Electronic Structure and Laser Foundation for Research and Technology Hellas, Heraklion, GreeceApplied Physics Department, Soreq Nuclear Research Center, Yavne, IsraelApplied Physics Department, Soreq Nuclear Research Center, Yavne, IsraelAneutronic p-11B nuclear fusion is promising for clean energy production, as it produces three (3) alpha particles with 8.7 MeV total energy. However, the main difficulty for p-11B fusion ignition (Q = Pfus/PBrems≥ 1) concerns the nuclear cross section and thus, reactivity efficiency at higher than 200 keV medium temperatures. To overcome this difficulty, the present work emphasizes on the numerical investigation of medium schemes (configurations) with enhanced reactivity. The configurations refer to the addition of energetic protons in a low-density 11boron or proton–11boron medium (n = 1020 m−3), with (np/nB) > 1 for Bremsstrahlung losses optimization and initial temperature in the range of 1 keV ≤ Tin≤ 400 keV. A self-consistent multi-fluid global particle and energy balance code, including collisions between all medium species (p, 11B, e, α), is used for the description of the temporal evolution of all fusion medium physical parameters and the evaluation of the optimum initial conditions for the obtainment of Q ≥ 1. The numerical simulation results show that the coupling between the 200 keV < Ep,0≤ 750 keV energetic protons and the 1 keV ≤ Tin≤ 400 keV initial fusion medium leads to ignition, 1 ≤ Q < 1.4, below Tin= 100 keV. In all the presented initial medium temperature cases, and especially, the lower (<) than 100 keV, the ignition condition (Pfus/PBrems) > 1 arises, as a consequence of the chain reactions and the related avalanche alpha heating effect.https://www.frontiersin.org/articles/10.3389/fphy.2024.1425963/fullproton–boron fusionlow-density plasmaenergetic protons in low-density p-11B mediummulti-fluid codealpha heating effectchain reactions
spellingShingle C. Daponta
S. Moustaizis
S. Eliezer
Z. Henis
P. Lalousis
N. Nissim
Y. Schweitzer
Towards p-11B medium configurations with high Pfus/PBrems ratios
Frontiers in Physics
proton–boron fusion
low-density plasma
energetic protons in low-density p-11B medium
multi-fluid code
alpha heating effect
chain reactions
title Towards p-11B medium configurations with high Pfus/PBrems ratios
title_full Towards p-11B medium configurations with high Pfus/PBrems ratios
title_fullStr Towards p-11B medium configurations with high Pfus/PBrems ratios
title_full_unstemmed Towards p-11B medium configurations with high Pfus/PBrems ratios
title_short Towards p-11B medium configurations with high Pfus/PBrems ratios
title_sort towards p 11b medium configurations with high pfus pbrems ratios
topic proton–boron fusion
low-density plasma
energetic protons in low-density p-11B medium
multi-fluid code
alpha heating effect
chain reactions
url https://www.frontiersin.org/articles/10.3389/fphy.2024.1425963/full
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AT smoustaizis towardsp11bmediumconfigurationswithhighpfuspbremsratios
AT seliezer towardsp11bmediumconfigurationswithhighpfuspbremsratios
AT zhenis towardsp11bmediumconfigurationswithhighpfuspbremsratios
AT plalousis towardsp11bmediumconfigurationswithhighpfuspbremsratios
AT nnissim towardsp11bmediumconfigurationswithhighpfuspbremsratios
AT yschweitzer towardsp11bmediumconfigurationswithhighpfuspbremsratios