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12TH•Physics•Nuclear And Particle Physics•Mass Defect and Binding Energy

19.1 Mass Defect and Binding Energy

$\\Delta m$, $B.E. = \\Delta mc^{2}$, binding energy per nucleon, and Example 19.1.

19.1 Mass Defect and Binding Energy

The results of experiments on the masses of different nuclei show that the mass of the nucleus is always less than the total mass of all the protons and neutrons making up the nucleus. The lost or missing mass is called mass defect Δm\Delta m given by the equation:

Δm=[Zmp+(A−Z)mn]−mnucleus…(19.1)\Delta m = [Zm_{p} + (A - Z)m_{n}] - m_{\mathrm{nucleus}} \quad \ldots (19.1)

where mpm_{p} is the mass of a proton, mnm_{n} is the mass of a neutron and mnucleusm_{\mathrm{nucleus}} is the mass of the entire nucleus. The missing mass is converted to energy, used in the formation of the nucleus. This energy can be calculated from Einstein's mass-energy relation:

ΔE=(Δm)c2…(19.2)\Delta E = (\Delta m)c^{2} \quad \ldots (19.2)

this energy is the potential energy called the Binding Energy (B.E) of the nucleus. It is defined as:

The work done on the nucleus to break it into constituents neutrons and protons. Binding energy is considered to have negative value similar to absolute gravitational potential value taken as zero on the surface of the Earth. A better measure is the building energy per nucleon. It can be considered as the average energy needed to separate a nucleus into its individual nucleons (neutrons and protons).

We usually use the masses of sub-atomic particles in atomic mass unit (amu or u) which is 1/121/12th of the mass of an unbound natural atom of 612C_{6}^{12}\mathrm{C}. 1 u=1.66×10−27 g1\,\mathrm{u} = 1.66 \times 10^{-27}\,\mathrm{g} or 1 u=1.66×10−27 kg1\,\mathrm{u} = 1.66 \times 10^{-27}\,\mathrm{kg}

Example 19.1

Find the mass defect and binding energy of the helium nucleus given that; Mass of proton mp=1.672623×10−27 kgm_{p} = 1.672623 \times 10^{-27}\,\mathrm{kg} Mass of neutron mn=1.674929×10−27 kgm_{n} = 1.674929 \times 10^{-27}\,\mathrm{kg} Mass of nucleus =6.646786×10−27 kg= 6.646786 \times 10^{-27}\,\mathrm{kg}

Solution

Using mass defect equation: Δm=2mp+2mn−mnucleus\Delta m = 2m_{p} + 2m_{n} - m_{\mathrm{nucleus}} =2(1.672623)×10−27 kg+2(1.674929)×10−27 kg−6.646786×10−27 kg= 2(1.672623) \times 10^{-27}\,\mathrm{kg} + 2(1.674929) \times 10^{-27}\,\mathrm{kg} - 6.646786 \times 10^{-27}\,\mathrm{kg} =6.695104×10−27 kg−6.646786×10−27 kg= 6.695104 \times 10^{-27}\,\mathrm{kg} - 6.646786 \times 10^{-27}\,\mathrm{kg} Δm=0.048318×10−27 kg\Delta m = 0.048318 \times 10^{-27}\,\mathrm{kg} Using Einstein's Equation: B.E=Δmc2B.E = \Delta m c^{2} =0.048318×10−27 kg×(3.0×108 m s−1)2= 0.048318 \times 10^{-27}\,\mathrm{kg} \times (3.0 \times 10^{8}\,\mathrm{m\,s^{-1}})^{2} B.E=4.34862×10−12 JB.E = 4.34862 \times 10^{-12}\,\mathrm{J} Changing into eV\mathrm{eV} B.E=(4.34862×10−12 J)/(1.6×10−19 J (eV)−1)=27 MeVB.E = (4.34862 \times 10^{-12}\,\mathrm{J}) / (1.6 \times 10^{-19}\,\mathrm{J\,(eV)^{-1}}) = 27\,\mathrm{MeV}

For your Information

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Energy must be supplied to break the nucleus apart into its constituent protons and neutrons.

Some Atomic Masses

ParticleMass (u)
Neutron0.0086650.008665
Proton1.0086651.008665
1H^{1}\mathrm{H}1.0072761.007276
2H^{2}\mathrm{H}2.0141022.014102
3H^{3}\mathrm{H}3.016053.01605
3He^{3}\mathrm{He}3.016033.01603
4He^{4}\mathrm{He}4.0026034.002603
7Li^{7}\mathrm{Li}7.0160047.016004
10B^{10}\mathrm{B}10.01353410.013534
14N^{14}\mathrm{N}14.003114.0031
17O^{17}\mathrm{O}16.999116.9991

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