Structure of Nucleus (original) (raw)

Last Updated : 23 Jul, 2025

The nucleus of an atom consists of two types of particles, positively charged particles called protons and neutrally charged particles called neutrons. **Protons + Neutrons in an atom represent the nucleus of an atom. The nucleus of an atom is represented by ZXA, where X is the nucleus of an atom, Z is the atomic number and A is the mass number.

structure of nucleus

**Note: Few important points to remember regarding the nucleus are:

Types of Nuclei

Various types of Nuclei are discussed below:

Size of the Nucleus

Rutherford assumed the distance of the closest approach as a measure of the size of an atomic nucleus. Assuming, the nuclei are spherical, the relation between the radius of the nucleus and the mass number is given by:

**R = R 0 A 1/3

where,
**R 0 is constant
For electrons R0 = 1.25×10-15m = 1.25 fermi(fm)

The Radius R of a nucleus is proportional to the cube root of its mass number.

Density of Nucleus

The nuclear density is independent of mass number A. The nuclear density is nearly constant and is equal to

**ρ = (3m)/(4πR 0 3 ) = 2.04×10 17 kg/m 3

where **m is the mass of a nucleus

Atomic Mass Unit (u or amu)

One atomic mass unit is defined as (1/12)th of the actual mass of a carbon-12 atom. It is denoted by amu or u.

1 amu = (1/12)× Mass of carbon-12 atom

= (1/12) × 1.992678×10-26 kg

**1 amu = 1.660565×10 -27 kg

Electron Volt

It is defined as the energy acquired by an electron when it is accelerated through a potential difference of 1 volt and is denoted by eV.

**1 eV = 1.602×10 -19 J

**Relation between amu and MeV:

**1 amu = 931 MeV

**Nuclear Forces

The strong forces of attraction which firmly hold the nucleons in the small nucleus and account for the stability of the nucleus are called nuclear forces.

**Characteristics of Nuclear Force

Some important characteristics of Nuclear Forces are:

Mass Defect

The mass of the nucleus is always less than the sum of the masses of nucleons composing the nucleus. The difference between the rest mass of the nucleus and the sum of the rest masses of nucleons constituting the nucleus is known as mass defect.

**△m = [Zm p +(A-Z)m n ] - M( Z X A )

where,
**m p= mass of protons
**Z = Atomic number
**A = Mass number

Binding Energy

The energy required to break a nucleus into its constituent nucleons and place them at an infinite distance is called binding energy.

**BE = (△m) c 2 = c 2 [Zm p +(A-Z)m n - M( Z X A )]

where,
**m p = mass of protons
**Z = Atomic number
**A = Mass number
**c = speed of light

**Rest Mass of Protons + Rest Mass of Neutrons = Rest Mass of Nucleus + BE

Binding Energy per Nucleon

The binding energy per nucleon of a nucleus is the average energy required to extract a nucleon from the nucleus.

Binding energy per nucleon \bar{B}= \frac{\text{Total binding energy}}{\text{Total number of nucleons} }=\frac{BE}{A}=\frac{\triangle mc^2}{A}

Solved Examples of Structure of Nucleus

**Example 1: Compare the radii of two nuclei with mass numbers 1 and 27 respectively.

**Solution:

Radius of nucleus R = R0A1/3

\frac{R_1}{R_2}= \big(\frac{A_1}{A_2}\big)^{1/3}

R1/R2 = (1/27)1/3

= 1/3

**Example 2: What is the nuclear radius of **125 Fe if that of 27 Al is 3.6 fermi?

**Solution:

Nuclear radius, R = R0A1/3 ⇒ R∝A1/3

For Al, A = 27, RAl = 3.6 fermi,

For Fe A = 125

\frac{R_{Fe}}{R_{Al}}= \big(\frac{A_{Fe}}{A_{Al}}\big)^{1/3}

RFe/RAl = (125/27)1/3

RFe = (5/3)RAl

= (5/3) ×3.6 fermi

RFe = 6 fermi

**Example 3: A neutron breaks into a proton and electron. Calculate the energy produced in this reaction in MeV. Mass of an electron = 9.1 ×10 -31 kg, Mass of proton = 1.6725×10 -27 kg, Mass of neutron 1.6747×10 -27 kg. Speed of light = 3×10 8 ms -1 .

**Solution:

Mass defect (**)m = Mass of neutron - (mass of proton + mass of electron)

**m = [(1.6747×10-27) - (1.6725×10-27 + 9.1 ×10-31)]

**m = 0.0013×10-27 kg

Energy released Q = **mc2

Q = (0.0013×10-27) × (3×108)2

= 1.17×10-13 J

Q = (1.173×10-13) / (1.6×10-19)

= 0.73×106 eV

Q = 0.73 MeV

**Example 4: Find the binding energy of 12 6 C. Also, find the binding energy per nucleon. Given mass of **1 1 H = 1.0078 u, 10n =1.0087 u, **12 6 C = 12.00004u.

**Solution:

One atom of 126C consists of 6 protons, 6 electrons, and 6 neutrons. The mass of the uncombined protons and electrons is the same as that of six 11H atoms.

Mass of six 11H atoms = 6×1.0078 = 6.0468 u

Mass of six neutrons = 6 × 1.0087 = 6.0522 u

Total mass of particles = 6.0468 +6.0522
= 12.0990 u

Mass of 126C atom = 12.00004

Mass defect = 12.0990 - 12.00004
= 0.0990

Binding energy = 931 × (0.099)
= 92 MeV

Binding energy per nucleon = 92/12
= 7.66 MeV