The liquid drop model was proposed by George Gasmow in 1929, and developed by Niels Bohr and Carl Friedrich Von Weizsacher in 1935.
As a first approximation, we can think of a nucleon in a nucleus interacting with its nearest neighbor, similar to that of a molecule in a drop of liquid that is free to move while maintaining a fixed intermolecular distance.The energy E V is called the Volume Energy of a nucleus and is directly proportional to A.
The more the total number of nucleons, the more difficult it becomes to remove an individual nucleon from the nucleus. This energy corresponds to the amount of heat energy required to transform a liquid to its vapor state being proportional to the mass of a liquid.T he negative energy ES is called the Surface Energy of a nucleus. It is most significant for the lighter nuclei since a greater fraction of their nucleons are on the surface.
E C = Z(Z-1) / 2 V = - Z(Z-1)e 2 /8 πε 0 (1R)
Hence,
E C = - a 3 Z(Z-1)/ A 1/3
The Coulomb energy is negative because it arises from an effect that opposes nuclear stability. The Total Binding Energy Eb of a nucleus comes out to be the sum of its Volume, Surface, and Coulomb Energies:E b = E V + E S + E C = a 1 A - a 2 A 2/3 - a 3 Z(Z-1)/ A 1/3
Correction to the Formula:
The Binding energy formula can be corrected by taking into account two effects that do not fit into the simple Liquid Drop Model but which make sense in terms of a model that provides for nuclear energy levels. One of these effects occurs when the neutrons in a nucleus outnumber the protons, which means higher energy levels have to be occupied rather than the case if N and Z were equal.E a = - a 4 (N - Z)2A
Ea = - a 4 (A-2Z) 2 /A
The Asymmetry Energy is negative because it reduces the Binding Energy of the Nucleus.