Mass Defect And Nuclear Binding Energy (Copy)
• Energy–Mass Equivalence: E = mc²
- Mass and energy are interchangeable, as stated by Einstein’s equation:
E = mc²
where:
E = energy (Joules)
m = mass (kg)
c = speed of light in vacuum = 3.00 × 10⁸ m/s - A small amount of mass corresponds to a large amount of energy.
• Nuclear Reactions Representation
- Reactions are written in the form:
⁷₃Li + ⁴₂He → ⁸₄Be + ¹₁H - Superscript = nucleon number (mass number)
- Subscript = proton number (atomic number)
- Both nucleon and proton numbers must balance on both sides of the equation.
• Mass Defect (Δm)
- The mass of a nucleus is less than the sum of the masses of its individual nucleons.
- This missing mass is the mass defect:
Δm = (Z × m_p) + (N × m_n) – m_nucleus
where:
Z = number of protons
N = number of neutrons
m_p = mass of proton
m_n = mass of neutron
m_nucleus = actual mass of the nucleus
• Binding Energy (BE)
- Binding energy is the energy required to separate a nucleus into its individual nucleons.
- It is also the energy released when a nucleus is formed from separate nucleons.
- Binding energy is related to mass defect by:
E = Δm × c²
(E in Joules when Δm in kg; use 1 u = 1.66 × 10⁻²⁷ kg if using atomic mass units)
• Binding Energy per Nucleon
- Defined as:
BE per nucleon = Total binding energy ÷ Number of nucleons - Useful for comparing nuclear stability.
- Greater BE per nucleon ⇒ more stable nucleus
• Graph: Binding Energy per Nucleon vs Nucleon Number
- Curve shows:
- Low BE/nucleon for light nuclei (e.g. hydrogen)
- Rapid rise for elements up to iron (Fe, A ≈ 56)
- Peak at iron-56 (most stable nucleus)
- Gradual decrease for heavy elements (e.g. uranium)
• Nuclear Fission
- Definition: A heavy nucleus (e.g. ²³⁵₉₂U) splits into two smaller nuclei, releasing energy.
- Mass of products < Mass of reactants ⇒ mass defect → energy release
- Used in nuclear reactors and atomic bombs.
• Nuclear Fusion
- Definition: Two light nuclei (e.g. ¹₁H + ¹₁H) combine to form a heavier nucleus, releasing energy.
- More energy released than fission (per unit mass).
- Requires very high temperature and pressure due to repulsive electrostatic forces.
- Powers stars like the Sun.
• Relevance of Binding Energy per Nucleon
- In fusion, small nuclei combine to form one with higher BE per nucleon, releasing energy.
- In fission, large nucleus splits into ones with higher BE per nucleon, also releasing energy.
- Energy comes from the increase in total BE.
• Calculating Energy Released in Nuclear Reactions
- Step 1: Find mass defect:
Δm = Total mass of reactants – Total mass of products - Step 2: Convert Δm to kg if given in atomic mass units (1 u = 1.66 × 10⁻²⁷ kg)
- Step 3: Use:
E = Δm × c²
or, for quick calculation in MeV:
1 u ≈ 931.5 MeV
⇒ E (MeV) = Δm (u) × 931.5
Worked Example
Given: Mass of reactants = 4.032 u, mass of products = 4.0026 u
Δm = 4.032 – 4.0026 = 0.0294 u
Energy released = 0.0294 × 931.5 = 27.4 MeV
Written and Compiled By Sir Hunain Zia, World Record Holder With 154 Total A Grades, 7 Distinctions and 11 World Records For Educate A Change A2 Level Physics Full Scale Course
