Suppose electron scattering fixes the radius parameter at instead of the value used…

PHYSICS · Multi-part · Fermi University Physics · Nuclear Physics · Nuclear constituents, size and binding · Nuclear constituents, size and binding

The Nucleus Resolved, Ch How big a nucleus is, and what the mass surface knows

Problem

Suppose electron scattering fixes the radius parameter at r0=1.25 fmr_0 = 1.25\,\mathrm{fm} instead of the value used in the refitted mass formula. ((a)) Recompute the Coulomb coefficient aC=35(e2/4πϵ0)/r0a_C = \tfrac{3}{5}(e^2/4\pi\epsilon_0)/r_0 for this r0r_0. ((b)) Using this aCa_C together with the other refitted coefficients aV=15.76 MeVa_V = 15.76\,\mathrm{MeV}, aS=17.91 MeVa_S = 17.91\,\mathrm{MeV}, aA=23.25 MeVa_A = 23.25\,\mathrm{MeV}, aP=12.51 MeVa_P = 12.51\,\mathrm{MeV}, compute the predicted binding energy of 40Ca^{40}\mathrm{Ca} (Z=N=20Z=N=20) from the semi-empirical mass formula B=aVA−aSA2/3−aCZ(Z−1)/A1/3−aA(N−Z)2/A+δB=a_VA-a_SA^{2/3}-a_CZ(Z-1)/A^{1/3}-a_A(N-Z)^2/A+\delta, with δ=+aP/A\delta=+a_P/\sqrt{A} for even-even nuclei, and compare it with the measured value B(40Ca)=342.1 MeVB(^{40}\mathrm{Ca}) = 342.1\,\mathrm{MeV} to find the binding-energy residual.

Related theory

Browse the problem library