{"id":1323,"date":"2021-03-11T07:38:10","date_gmt":"2021-03-11T12:38:10","guid":{"rendered":"http:\/\/www.journal-of-nuclear-physics.com\/?p=1323"},"modified":"2021-03-11T07:38:10","modified_gmt":"2021-03-11T12:38:10","slug":"on-the-role-of-nuclear-binding-energy-in-understanding-cold-nuclear-fusion","status":"publish","type":"post","link":"https:\/\/www.journal-of-nuclear-physics.com\/?p=1323","title":{"rendered":"On the Role of Nuclear Binding Energy in Understanding Cold Nuclear Fusion"},"content":{"rendered":"

.<\/span>
\nby<\/em>
\nU.V.S.Seshavatharam and S.Lakshminarayana<\/em>
\nHonorary faculty, I-SERVE, Survey no-42, Hitech city, Hyderabad-84,Telangana, INDIA<\/em>
\nDept.of Nuclear Physics, Andhra University, Visakhapatnam-03, AP, INDIA<\/em>
\nEmails: seshavatharam.uvs@gmail.com (and) lnsrirama@gmail.com<\/em>
\nOrcid numbers: 0000-0002-1695-6037 (and) 0000-0002-8923-772X<\/em><\/p>\n

.<\/span>
\nRead the whole article<\/a>
\nDownload the ZIP file<\/a>
\n.<\/span><\/p>\n

Abstract<\/strong>
\nFollowing the concept of strong interaction, theoretically, fusion of proton seems to increase the binding energy of final atom by 8.8 MeV.
\nDue to Coulombic repulsion, asymmetry effect, pairing effect and other nuclear effects, final atom is forced to choose a little bit of binding energy less than 8.8 MeV and thus it is able to release left over binding energy in the form of internal kinetic energy or external thermal energy.
\nThus, in cold fusion, heat release to occur, binding energy difference of final atom and base atom seems to be less than 8.8 MeV.
\nQualitatively, energy released during cold fusion seems to be approximately equal to 8.8 MeV minus the difference of binding energy of final and base atoms.
\nBased on this idea, under normal conditions, for the case of 2He4, fusion of four protons can liberate (35.2-28.3)=6.9 MeV and it is 3.5 times less than the current estimates.
\nPoint to be understood is that, lesser the binding energy of final atom, higher the liberated thermal energy and vice versa.
\nWith a suitable catalyst and sufficient hydrogen under suitable pressure, if reactor\u2019s temperature is maintained at (1000 to 1500) 0C, there seems a lot of scope for a chain reaction of cold fusion in which light isotopes transform to their next stage with increased proton number or mass number and liberate safe and clean heat energy continuously.
\nBy arranging 4 to 6 reactors and charging them periodically in tandem, required thermal energy can be produced continuously.
\nIn this new direction, by carefully selecting the base isotope and its corresponding catalyst, experiments can be conducted and ground reality of cold fusion can be understood at various temperature and pressure conditions.
\n.<\/span>
\nRead the whole article<\/a>
\nDownload the ZIP file<\/a>
\n.<\/span><\/p>\n","protected":false},"excerpt":{"rendered":"

. by U.V.S.Seshavatharam and S.Lakshminarayana Honorary faculty, I-SERVE, Survey no-42, Hitech city, Hyderabad-84,Telangana, INDIA Dept.of Nuclear Physics, Andhra University, Visakhapatnam-03, AP, INDIA Emails: seshavatharam.uvs@gmail.com (and) lnsrirama@gmail.com Orcid numbers: 0000-0002-1695-6037 (and) 0000-0002-8923-772X<\/p>\n

. Read the whole article Download the ZIP file .<\/p>\n

Abstract Following the concept of strong interaction, theoretically, […]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":[],"categories":[3],"tags":[],"_links":{"self":[{"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=\/wp\/v2\/posts\/1323"}],"collection":[{"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=1323"}],"version-history":[{"count":1,"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=\/wp\/v2\/posts\/1323\/revisions"}],"predecessor-version":[{"id":1324,"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=\/wp\/v2\/posts\/1323\/revisions\/1324"}],"wp:attachment":[{"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=1323"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=1323"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.journal-of-nuclear-physics.com\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=1323"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}