<p>The features of high-gain aneutronic p–<sup>11</sup>B fusion are examined. A comparison of inertial systems with extremely high plasma densities (<i>n</i> ~ 10<sup>30</sup>–10<sup>31</sup>&#xa0;m<sup>–3</sup>) and stationary systems with magnetic confinement of low-density plasma (<i>n</i> ~ 10<sup>20</sup>–10<sup>22</sup>&#xa0;m<sup>–3</sup>) shows that it is also necessary to analyze combined schemes based on magneto-inertial systems with fuel refill. Present work considers limiting modes of the quasi-stationary phase of fusion, which show the maximum plasma gain at plasma density <i>n</i> ~ 10<sup>31</sup>&#xa0;m<sup>–3</sup> and ion temperatures <i>T</i><sub><i>i</i></sub> ~ 200&#xa0;keV, electron temperatures <i>T</i><sub><i>e</i></sub> ~ 100&#xa0;keV at the beginning of the quasi-stationary phase. The content of reaction products (α-particles) has a significant influence on the parameters of the system. If the confinement time of α-particles is the same as for the fuel components, then due to radiation the energy gain <i>Q</i> ~ 1. In modes with a reduced confinement time of α-particles, the gain reaches a value of <i>Q</i> ~ 6. A further increase in <i>Q</i> requires extremely high plasma energy.</p>

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Power Balance of the Quasi-Stationary Stagnation Phase of Superdense Boron-Proton Plasma

  • Alexei Yu. Chirkov,
  • Evgeny G. Vovkivsky

摘要

The features of high-gain aneutronic p–11B fusion are examined. A comparison of inertial systems with extremely high plasma densities (n ~ 1030–1031 m–3) and stationary systems with magnetic confinement of low-density plasma (n ~ 1020–1022 m–3) shows that it is also necessary to analyze combined schemes based on magneto-inertial systems with fuel refill. Present work considers limiting modes of the quasi-stationary phase of fusion, which show the maximum plasma gain at plasma density n ~ 1031 m–3 and ion temperatures Ti ~ 200 keV, electron temperatures Te ~ 100 keV at the beginning of the quasi-stationary phase. The content of reaction products (α-particles) has a significant influence on the parameters of the system. If the confinement time of α-particles is the same as for the fuel components, then due to radiation the energy gain Q ~ 1. In modes with a reduced confinement time of α-particles, the gain reaches a value of Q ~ 6. A further increase in Q requires extremely high plasma energy.