Nuclear Physics Fundamentals
Nuclear Fission
Nuclear fission is the process where a heavy atomic nucleus splits into two or more smaller nuclei, along with free neutrons and a tremendous amount of energy. This is the fundamental process behind the first generation of nuclear weapons.
The Fission Process
- A neutron strikes a fissile nucleus (like Uranium-235 or Plutonium-239)
- The nucleus becomes unstable and splits into two smaller nuclei
- 2-3 additional neutrons are released
- Enormous energy is released (about 200 MeV per fission)
- Released neutrons can trigger more fissions, creating a chain reaction
Critical Mass
For a sustained chain reaction to occur, there must be enough fissile material present - this is called the critical mass. Below critical mass, too many neutrons escape without causing additional fissions. The critical mass depends on:
- The type of fissile material (U-235 vs Pu-239)
- The purity of the material
- The geometry and density
- The presence of neutron reflectors
Fissile Materials
Uranium-235
Critical mass: ~52 kg (bare sphere)
Natural abundance: 0.7%
Requires enrichment for weapons
Plutonium-239
Critical mass: ~10 kg (bare sphere)
Artificially produced in reactors
More efficient than U-235
Nuclear Fusion
Nuclear fusion is the process where light atomic nuclei combine to form heavier nuclei, releasing even more energy per unit mass than fission. This powers the sun and thermonuclear (hydrogen) bombs.
Fusion Reactions in Weapons
The primary fusion reactions used in thermonuclear weapons are:
- Deuterium + Tritium → Helium-4 + neutron + 17.6 MeV
- Deuterium + Deuterium → Tritium + proton + 4.0 MeV
- Deuterium + Deuterium → Helium-3 + neutron + 3.3 MeV
Conditions Required
Fusion requires extreme conditions to overcome the electrostatic repulsion between nuclei:
- Temperature: 50-100 million Kelvin
- Pressure: Millions of atmospheres
- Sufficient density and confinement time
In weapons, these conditions are achieved using a fission bomb as a "primary" to compress and heat the fusion fuel in the "secondary" stage.
Fusion Fuels
Deuterium (²H)
Heavy hydrogen isotope
Abundant in seawater
Relatively easy to obtain
Tritium (³H)
Radioactive hydrogen isotope
Half-life: 12.3 years
Must be artificially produced
Lithium-6
Used to breed tritium in situ
Enables "dry" fusion weapons
More practical for weapons
Thermonuclear Weapons Design
Modern thermonuclear weapons use a two-stage design called the Teller-Ulam configuration, which can achieve virtually unlimited yields.
Primary Stage (Fission)
- Plutonium or highly enriched uranium core
- Conventional explosives for implosion
- Provides X-rays and neutrons for secondary
- Typical yield: 10-50 kilotons
Secondary Stage (Fusion)
- Fusion fuel (lithium deuteride)
- Uranium tamper/pusher
- Radiation case for X-ray compression
- Can achieve megaton yields
Energy Distribution
In a typical thermonuclear weapon:
- ~50% from fusion reactions
- ~35% from fast fission in uranium tamper
- ~15% from primary fission trigger
Energy Release Comparison
Reaction Type | Energy per Reaction | Energy per kg | Example |
---|---|---|---|
Chemical (TNT) | ~4 eV | 4.6 MJ/kg | Conventional explosives |
Nuclear Fission | ~200 MeV | 80 TJ/kg | Hiroshima bomb |
Nuclear Fusion | ~17.6 MeV | 340 TJ/kg | Hydrogen bombs |
Note: TJ = Terajoule (10¹² joules), MJ = Megajoule (10⁶ joules)
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