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

  1. A neutron strikes a fissile nucleus (like Uranium-235 or Plutonium-239)
  2. The nucleus becomes unstable and splits into two smaller nuclei
  3. 2-3 additional neutrons are released
  4. Enormous energy is released (about 200 MeV per fission)
  5. 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 TypeEnergy per ReactionEnergy per kgExample
Chemical (TNT)~4 eV4.6 MJ/kgConventional explosives
Nuclear Fission~200 MeV80 TJ/kgHiroshima bomb
Nuclear Fusion~17.6 MeV340 TJ/kgHydrogen bombs

Note: TJ = Terajoule (10¹² joules), MJ = Megajoule (10⁶ joules)

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