The "binding energy" of a nucleus is the total energy of the bonds between the nucleons (the protons and neutrons) in the nucleus. Consider a neutral atom with Z protons and N neutrons in the nucleus, and let the total nucleon number A be given by A = Z + N . The binding energy can be written as a function of Z and A as:
E ( A , Z ) = a v A − a s A 2 / 3 − a c Z 2 A − 1 / 3 − a a ( A − 2 Z ) 2 A − 1 / 4 + δ A − 1 / 2 .
The values for the parameters in the above equation are a v = 1 5 . 6 7 MeV , a s = 1 7 . 2 3 MeV , a c = 0 . 7 1 4 MeV , a a = 9 3 . 1 5 MeV .
δ can take different values depending on whether A and Z are even or odd. To simplify the calculation, we'll let δ = 0 , which is one of the allowed values.
The nucleus is the most stable when the binding energy is highest, as that's when it takes the most energy to rip it apart. When A is small, we get Z = A / 2 for the most stable nuclei, and this explains why for lighter atoms half of the nucleus is generally protons and the other half is made from neutrons. When A is large, the most stable nuclei (the ones with highest binding energy) have Z ∼ A 1 − y = A w . Find w .
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OK, cool, this is a brute-force problem: we just need to find the value of Z to maximize E ( A , Z ) with the value of A fixed by setting the derivative of E ( A , Z ) with respect to Z equal to 0 . The final result is pretty straightforward: Z = 2 a a a c A 2 / 3 + 2 A With large A , Z = 2 a c a a A 1 / 3 , so w = 1 / 3 .
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for an element with given value of A,for binding energy to be maximum
differentiation of E w.r.t Z keeping A constant must be Zero.
i.e. - 2a cZA^{-1/3} + a a{A-2Z}A^{-1} = 0
which gives Z=a a A / { 2a a + 2a_cA^{2/3} }
since a c is very much less than a a. so for elements with low mass number(A),second term of denominator can be neglected giving
Z=A/2,
But in case of elements with high mass number,the things are opposite
here first term of denominator is neglected giving
Z ~ A^{1 - 1/3} = A^{0.333}