N. Niknam, S. N. Hosseinimotlagh, M. Eshghi, Z. Parang
{"title":"Role of a helium catalyzed process and deuteron beam radiation simultaneously on the D3He target to create supplementary fusion energy","authors":"N. Niknam, S. N. Hosseinimotlagh, M. Eshghi, Z. Parang","doi":"10.1007/s40042-025-01309-6","DOIUrl":null,"url":null,"abstract":"<div><p>The energy enhancement required for fusion through ICF can be achieved through fast ignition as a good method. The use of deuteron beams and injected into the fusion plasma containing D<sup>3</sup>He increases the amount of fusion reactor fuel and the deuteron beam causes the fast ignition. The incident deuteron beam stopping power in the desired fusion plasma is higher than that of the electron. Therefore, they can create a higher energy density by stopping at a smaller volume of fuel, and it produces supplementary energy. Note that another advantage of using a deuteron beam is that it reduces the energy of the required laser beams. This issue can play a significant role in increasing the efficiency of commercial fusion reactors. In this work, we have calculated the amount of deposited energy or the produced supplementary energy due to deuteron beam radiation and performing fusion reactions. However, in the ICF approach, using pure D<sup>3</sup>He fuel is impractical due to the excessive requirement for ignition energy. Therefore, a small amount of DT fuel is necessary as an “igniter”. Since the D<sup>3</sup>He reaction does not produce any neutrons and the fuel sources of the DD fusion reaction are available in sufficient quantity in Earth, it is expected that these reactions can be used as a source of clean energy. The process of helium catalyzed D<sup>3</sup>He is the primary focus of advanced fuel fusion reactors. In this article, we determined the fusion energy gain, G, from the solving of time-dependent non-linear point kinetic differential equations coupled together for two processes with and without helium catalyzed process. The results of this study have shown that G gradually increases with increasing temperature, and at a temperature of 190 keV, the value of G reaches its maximum value, so that at this temperature, for the two states without and with the helium catalyzed process, the G value reaches about 20 and 110, respectively, which shows that considering the helium catalyzed process simultaneously deuteron beam radiation provides access to supplementary energy and finally G increases.</p></div>","PeriodicalId":677,"journal":{"name":"Journal of the Korean Physical Society","volume":"86 7","pages":"636 - 648"},"PeriodicalIF":0.8000,"publicationDate":"2025-02-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of the Korean Physical Society","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.1007/s40042-025-01309-6","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
The energy enhancement required for fusion through ICF can be achieved through fast ignition as a good method. The use of deuteron beams and injected into the fusion plasma containing D3He increases the amount of fusion reactor fuel and the deuteron beam causes the fast ignition. The incident deuteron beam stopping power in the desired fusion plasma is higher than that of the electron. Therefore, they can create a higher energy density by stopping at a smaller volume of fuel, and it produces supplementary energy. Note that another advantage of using a deuteron beam is that it reduces the energy of the required laser beams. This issue can play a significant role in increasing the efficiency of commercial fusion reactors. In this work, we have calculated the amount of deposited energy or the produced supplementary energy due to deuteron beam radiation and performing fusion reactions. However, in the ICF approach, using pure D3He fuel is impractical due to the excessive requirement for ignition energy. Therefore, a small amount of DT fuel is necessary as an “igniter”. Since the D3He reaction does not produce any neutrons and the fuel sources of the DD fusion reaction are available in sufficient quantity in Earth, it is expected that these reactions can be used as a source of clean energy. The process of helium catalyzed D3He is the primary focus of advanced fuel fusion reactors. In this article, we determined the fusion energy gain, G, from the solving of time-dependent non-linear point kinetic differential equations coupled together for two processes with and without helium catalyzed process. The results of this study have shown that G gradually increases with increasing temperature, and at a temperature of 190 keV, the value of G reaches its maximum value, so that at this temperature, for the two states without and with the helium catalyzed process, the G value reaches about 20 and 110, respectively, which shows that considering the helium catalyzed process simultaneously deuteron beam radiation provides access to supplementary energy and finally G increases.
期刊介绍:
The Journal of the Korean Physical Society (JKPS) covers all fields of physics spanning from statistical physics and condensed matter physics to particle physics. The manuscript to be published in JKPS is required to hold the originality, significance, and recent completeness. The journal is composed of Full paper, Letters, and Brief sections. In addition, featured articles with outstanding results are selected by the Editorial board and introduced in the online version. For emphasis on aspect of international journal, several world-distinguished researchers join the Editorial board. High quality of papers may be express-published when it is recommended or requested.