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Relationship between nuclear binding energy (B) and mass defect ( D ). B (Z,A) = [Zm (1H) +Nm n – M (Z,A) ]c 2 D = [M (Z,A) – A]c 2 all masses in atomic mass units (u) B + D = [ Zm (1H) +Nm n – A]c 2 = [Z(1.007825) + N(1.008665) – Z – N]c 2
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Relationship between nuclear binding energy (B) and mass defect (D) B (Z,A) = [Zm(1H) +Nmn – M(Z,A)]c2 D = [M(Z,A) – A]c2 all masses in atomic mass units (u) B + D = [Zm(1H) +Nmn – A]c2 = [Z(1.007825) + N(1.008665) – Z – N]c2 = [Z(0.007825) + N(0.008665)]c2
Nuclear radii Nuclei have nearly constant density A/(4/3)pR3 ~ constant R a A1/3 R = R0 A1/3 ,with R0 = 1.2 fm
Quantum MechanicsKrane: Chapter 2 The Infamous Double Slit Experiment http://www.youtube.com/watch?v=wEzRdZGYNvA
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