1.The Bethe-Weizsacker formula:
m=Zmp+(A−Z)mn−c21[aVA−aSA2/3−aCA1/3Z(Z−1)−aAA(A−2Z)2] where mp,mn,aV,aS,aC,aA are positive constants (can be taken from the https://en.wikipedia.org/wiki/Semi-empirical_mass_formula#Calculating_the_coefficients).
Let's differenciate this expression wrt to Z and equate the derivative to zero:
dZdm=mp−mn−c21[−aCA1/32Z−1+aAA4(A−2Z)]=0 Expressing Z from this equation:
−aCA1/32Z−aAA8Z=c2(mp−mn)−aCA1/31−4aAZ(A1/32aC+A8aA)=c2(mn−mp)+A1/3aC+4aAZmin=2aC+8aA4AaA+Ac2(mn−mp)+A2/3aC Let's check wheather this value gives us minimal m. The second derivative:
dZ2d2m=(A1/32aC+A8aA)>0 Thus the m(Zmin,A) is the minimal value indeed.
2. As far as A=N+Z the obtained vlaue for Zmin gives some region on the (Z,N) graph with the mnimal value of m, which is called 'valley of beta stability'.
3. For A = 16 the stablest nucleus will be:
Zmin=2⋅0.71+8⋅23.24⋅16⋅23.2+16⋅c2(938.57MeV/c2−938.3MeV/c2)+162/3⋅0.71==7.98≈8
Thus, the most stable nucleus at A = 16 is the nucleus of 16O
For A = 208:
Zmin=2⋅0.71+8⋅23.24⋅208⋅23.2+208⋅c2(938.57MeV/c2−938.3MeV/c2)+2082/3⋅0.71==103.64≈104 Thus, the most stable nucleus at A = 208 is the nucleus of 208Rf.
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