We are given the following atomic masses: `._92U^(238)=238.05079u,` `._90Th^(234)=234.04363u`, `._91Pa^(237)=237.05121, ._1H^1=1.00783`, `._2He^2=4.00260u` (a) Calculate the energy released during `alpha` decay of `._92U^(238)`, (b) Calculate the kinetic energy of emitted `alpha` particles, (c) show that `._94U^(238)` cannot spontaneously emit a proton.
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The equation representing `alpha` decay of `._92U^(238)` is `._92U^(238)to ._90Th^(234)+._2He^4+Q`, where Q is the kinetic energy shared by Th & He. Mass defect in the decay process is `Deltam =m(._92U^(238))-m(._90Th^(234))-m(._2He^4)` `=238.05081-234.04363-4.00260` `=0.00458 a.m.u` `:. Q=0.00458xx931MeV` `=4.26 MeV` This is shared between Th &He. As He is much ligther compared to Th, therefore, most of this energy is K.E. of He alone.
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