>>
Study Material >>
IIT JEE Physics >>
Modern Physics >>
Structure of Atom and Nucleus >>
Mass Defect and Binding Energy
Mass Defect Binding Energy
The nucleons are bound together in a nucleus and the energy has to be supplied in order to break apart the constituents into free nucleons. The energy with which nucleons are bounded together in a nucleus is called as Binding Energy (B.E.). In order to free nucleons from a bounded nucleus this much of energy (= B.E.) is to be supplied.
It is observed that the mass of a nucleus is always less than the mass of constituent (free) nucleons. This difference in mass is called as mass defect and is denoted as Dm.
If mn: mass of a neutron;
mp: mass of a proton
M (Z, A): mass of bounded nucleus
Then, Δm = Z . mp + (A – Z). mn – M (Z, A)
This mass-defect is in form of energy and is responsible for binding the nucleons together. From Einstein's law of inter-conversion of mass into energy:
E = mc2 (c: speed of light; m: mass)
binding energy = Δm . c2
Generally, Δm is measured in amu units. So let us calculate the energy equivalent to 1 amu. It is calculated in eV (electron volts; 1 eV =1.6 x10–19J)
E (= 1 amu = 1.67 × 10–27 (3×108)2 / 1.6 × 10–19) eV = 931 × 108 eV = 931 MeV
=> B.E. = Δm (931) MeV
There is another quantity which is very useful in predicting the stability of a nucleus called as Binding energy per nucleons.
B.E. per nucleons = Δm (931) / A MeV

From the plot of B.E./nucleons Vs mass number (A), we observe that:
(i) B.E./nucleons increases on an average and reaches a maximum of about 8.7 MeV for A º 50 – 80.
(ii) For more heavy nuclei, B.E./nucleons decreases slowly as A increases. For the heaviest natural element U238 it drops to about 7.5 MeV.
(iii) From above observation, it follows that nuclei in the region of atomic masses 50-80 are most stable.
Illustration 2:
If mass of proton = 1.008 amu and mass of neutron = 1.009 amu, then the binding energy per nucleon for 4Be9 (mass = 9.012 amu) will be:
(A) 0.0672 MeV (B) 0.672 MeV
(C) 6.72 MeV (D) 67.2 MeV
Solution:
Mass defect
Δm = (4 × 1.008 + 5 × 1.009) – 9.012
= 9.077 – 9.012 =0.065 amu
BE/A = 0.065 × 931 / 9 = 6.72 MeV
Illustration 4:
The energy released in the following b-decay process will be:

Given that
mn = 1.6747 × 10–27 kg
mp = 1.6725 × 10–27 kg
me = 0.00091 × 10–27 kg
(A) 0.931 MeV (B) 0.731 MeV
(C) 0.511 MeV (D) 0.271 MeV
Solution:
Mass defect Δm = (1.6747 – 1.6725 – 0.0091) × 10–27
= 0.0012 × 10–27 kg
ΔE = 0.0012 × 10–27 × (3 × 108)2 / 1.6 × 10–12 = 0.731 MeV
Illustration 5:
The binding energy per nucleon for 3Li7 will be, if the mass of 3Li7 is 7.01653 amu.
(A) 5.6 MeV (B) 39.25 MeV
(C) 1 MeV (D) zero.
Solution:
E =
ΔE / A =
Δm × 931 / A MeV
Δm = (3mp + 4mn) – mass of Li7
= (3 × 1.00759 + 4 × 1.008898) – 7.01653
= 0.04216
ΔE = 0.04216 × 931 / 7 = 39.25 / 7 = 5 MeV
Illustration 6:
How much energy is released in the following reaction?
1H2 + 1H2 = 2He4
If the B.E./Nucleon of 1H2 and 2He4 are 1.123 MeV and 7.2 MeV respectively.
(A) 12 MeV (B) 24.3 MeV
(C) 36 MeV (D) zero
Solution:
B. E. of 1H2
ΔE = 1.125
E = A × ΔE
E = 2 × 1.125
= 2.25 MeV
B.E. of two 1H2 = 2.25
Ed = 4.5 MeV
B.E. of an α -particle = 4 × 7.2
Ea = 28.8
Energy released ER = Ea – Ed
ER = 28.8 – 4.5 = 24.3 MeV