{"title":"Application of laser fusion to the production of fissile materials","authors":"R.N. Horoshko, H. Hurwitz , H. Zmora","doi":"10.1016/0302-2927(74)90035-X","DOIUrl":null,"url":null,"abstract":"<div><p>Calculations are made for the amount of <sup>239</sup>Pu produced and the number of fast fissions occuring per 14 MeV neutron in a medium containing various concentrations of <sup>238</sup>U, <sup>239</sup>Pu, <sup>16</sup>O, and <sup>23</sup>Na. Neutrons are assumed to be produced by a laser induced D + T fusion reaction and to interact with a blanket containing fertile materials where plutonium breeding occurs. Calculations show that in pure <sup>238</sup>U the neutron multiplication factor is 4·6 and that 1·08 fast fissions occur per each D + T reaction. Assuming a neutron production rate of 3 × 10<sup>19</sup> sec at <em>E</em><sub><em>n</em></sub> = 14 MeV and allowing for <sup>23</sup>Na cooling of the <sup>238</sup>U blanket, the thermal energy generated is nearly 1000 MW, while the thermal value of the produced <sup>239</sup>Pu is 4 times as large. Values are somewhat lower in cases where UO<sub>2</sub> is used in the blanket. Buildup of <sup>239</sup>Pu in the blanket is considered and is found to have the effect of strongly increasing both the net <sup>239</sup>Pu production and the thermal power generated.</p><p>Possibilities of using <sup>232</sup>Th in the blanket and the D + D fusion reaction are also discussed and are found to be energetically inferior.</p></div>","PeriodicalId":100094,"journal":{"name":"Annals of Nuclear Science and Engineering","volume":"1 3","pages":"Pages 223-232"},"PeriodicalIF":0.0000,"publicationDate":"1974-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0302-2927(74)90035-X","citationCount":"9","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Annals of Nuclear Science and Engineering","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/030229277490035X","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 9
Abstract
Calculations are made for the amount of 239Pu produced and the number of fast fissions occuring per 14 MeV neutron in a medium containing various concentrations of 238U, 239Pu, 16O, and 23Na. Neutrons are assumed to be produced by a laser induced D + T fusion reaction and to interact with a blanket containing fertile materials where plutonium breeding occurs. Calculations show that in pure 238U the neutron multiplication factor is 4·6 and that 1·08 fast fissions occur per each D + T reaction. Assuming a neutron production rate of 3 × 1019 sec at En = 14 MeV and allowing for 23Na cooling of the 238U blanket, the thermal energy generated is nearly 1000 MW, while the thermal value of the produced 239Pu is 4 times as large. Values are somewhat lower in cases where UO2 is used in the blanket. Buildup of 239Pu in the blanket is considered and is found to have the effect of strongly increasing both the net 239Pu production and the thermal power generated.
Possibilities of using 232Th in the blanket and the D + D fusion reaction are also discussed and are found to be energetically inferior.