MH

Nuclear Binding Energy and Nuclear Radiation

Nuclear Binding Energy and Mass Deficit

  • Experiments show the total mass of a nucleus is less than the sum of the masses of its constituent nucleons.

  • Mass Defect:

    • Defined as the difference between the measured mass of a nucleus and the total mass of its constituents.

    • Calculated using the formula:

    • \Delta m=Zmp+(A-Z)mn-mtotal

      • Where:

      • Z = proton number

      • A = nucleon number

      • mp = mass of a proton (kg)

      • mn = mass of a neutron (kg)

      • m{total} = measured mass of the nucleus (kg)

Mass-Energy Equivalence

  • A system of separated nucleons has a greater mass than that of bound nucleons.

  • Binding Energy:

    • The energy required to separate a nucleus into its individual protons and neutrons.

    • Formation of a nucleus from isolated nucleons releases energy, indicating it's an exothermic reaction.

    • Calculated using:

    • E = \Delta m \cdot c^2

      • Where:

      • E = energy (J)

      • m = mass (kg)

      • c = speed of light ($3.00 \times 10^8 \ m/s$)

  • Mass-Energy Equivalence:

    • Proposed by Einstein: Matter can become energy and vice versa.

  • Examples of mass-energy equivalence include:

    • Fusion of hydrogen into helium in stars.

    • Fission of uranium in nuclear power plants.

    • Nuclear explosions.

    • High-energy collisions in particle accelerators.

Atomic Mass Unit (a.m.u)

  • Unified atomic mass unit (u or a.m.u) is approximately the mass of one proton or neutron:

    • 1{ u}=1.66\times10^{-27}\text{ kg}

  • Defined as one-twelfth of a carbon-12 atom, which has a mass of exactly 12 u.

  • Since mass and energy are interchangeable:

    • 1{ u}=931.5ext{ MeV}

  • Practically used in nuclear physics for expressing the mass of subatomic particles.

Binding Energy per Nucleon

  • Defined as the total binding energy of a nucleus divided by the number of nucleons.

  • A higher binding energy per nucleon implies greater stability:

    • Iron (A = 56) has the highest binding energy per nucleon, making it the most stable element.

  • Key Features on Binding Energy Graph:

    • Low A values (light elements):

    • Lower binding energy per nucleon.

    • More likely to undergo fusion (e.g., Helium-4, Carbon-12).

    • Helium-4 is particularly stable.

    • High A values (heavy elements):

    • High initial binding energy per nucleon that gradually decreases with increasing A.

    • Heavier elements are typically less stable and likely to undergo fission.

Nuclear Fusion

  • Defined as the process where small nuclei combine to form larger nuclei, releasing energy.

  • Primarily occurs with low mass nuclei (like hydrogen and helium).

    • Example: Fusion of deuterium and tritium forms helium and releases energy.

Conditions for Nuclear Fusion
  • High kinetic energy required to overcome the electrostatic repulsion between protons:

    • Achievable in environments with temperatures around 100 \times 10^6 Kelvin.

  • Requires very high density.

Fusion Products
  • When two protons fuse, deuterium is produced.

  • In stellar cores, deuterium fuses with a tritium nucleus to create a helium nucleus and release energy, sustaining stellar processes.