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)
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.
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.
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.
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.
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.
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.