PHY 1020 – Chapter 5: Chain Reactions, Nuclear Reactors, and Atomic Bombs
Chain Reactions – Fundamental Concepts
- Definition: A chain reaction is a sequence of events in which one reaction initiates additional reactions, leading to a self-amplifying process.
- Mathematical growth law for binary chain reactions:
• Each event produces 2 new events → number of events after N steps is 2^N (law of doubling).
• Growth is exponential, not linear. - Physical requirements:
• A trigger event (e.g., neutron striking a fissile nucleus).
• Sufficient propagation medium (enough nuclei, cells, people, etc.).
• No dominant damping mechanism (losses, removal, exhaustion of resources).
Biological Analogies: Fetal Development & Cancer
- Human embryo/fetus as a biological chain reaction:
• One fertilized egg divides via mitosis → 2 → 4 → 8 … 2^N cells.
• Total cells in an adult ≈ 10^{11}.
• Solve 2^N = 10^{11} → N = \log_2 10^{11} \approx 11\times3.32 \approx 36.52 → about 37 cell-division days (idealized, ignores differentiation & apoptosis). - Cancer = “cells gone wild”:
• Uncontrolled mitotic chain reaction when regulatory mechanisms (immune surveillance, programmed cell death) fail.
• Younger/smaller bodies usually eliminate defective cells faster; loss of control → tumors.
• Illustrates why damping processes are vital to prevent runaway growth.
Population, Viral & Rumor Spread
- Human population growth shows near-exponential phases, but environmental carrying capacity limits sustainment (resource depletion, disease, social factors).
- Other self-propagating systems:
• Biological/computer viruses.
• Rumors & urban legends in social networks.
• Electron avalanche in lightning discharges.
Nuclear Fission Chain Reactions and Bomb Design
- Fissile isotopes: ^{235}\text{U} and ^{239}\text{Pu} naturally emit neutrons.
- Mechanism:
- Neutron absorbed → nucleus fissions → releases kinetic energy + \approx 2{-}3 fast neutrons.
- If >1 neutron on average induces new fission, reaction grows exponentially.
- Critical mass = minimum mass/geometry/density of fissile material needed so that each generation produces ≥1 subsequent fission.
• Depends on density, shape, purity (isotope ratio), neutron absorbers, and reflectors.
• Typical bare-sphere values (no reflector):
– Uranium-235: \approx 15\,\text{kg}.
– Plutonium-239: \approx 5\,\text{kg} (higher neutron yield & lower critical mass). - Two classic bomb architectures:
- Gun-type ("Little Boy") – Fires a hollow ^{235}\text{U} projectile into a ^{235}\text{U} target → super-critical mass; yield ≈ 15 kt.
- Implosion-type ("Fat Man") – Symmetric high-explosive lenses compress ^{239}\text{Pu} core → higher density lowers critical mass; yield ≈ 20 kt.
Thermonuclear (Fusion) Weapons
- Stage-1 fission device acts as trigger; Stage-2 fusion (deuterium + tritium or Li-6) yields vastly higher energy.
- “Hydrogen bomb” yields in megaton range; Hiroshima/Nagasaki become negligible by comparison.
- Example: USSR “Tsar Bomba” 50 Mt.
Effects Comparison: Hiroshima vs Tsar Bomba
- Hiroshima (15 kt):
• Fatalities ≈ 29,140; injuries ≈ 30,360.
• Destructive radius ≈ 1.91 km. - Tsar Bomba (50 Mt) modeled over Jacksonville, FL:
• Fatalities ≈ 633,650; injuries ≈ 347,040.
• Destructive radius ≈ 60 km. - Demonstrates cubic scaling of blast volume with yield.
Uranium Enrichment & Manhattan Project
- Natural uranium (~99.3 % ^{238}\text{U}, 0.7 % ^{235}\text{U}) too dilute for bombs/reactors.
- Converted to uranium hexafluoride (UF6) for gaseous diffusion or centrifuge separation.
- WWII K-25 plant (Oak Ridge, TN) produced highly enriched uranium shipped to Los Alamos for bomb assembly.
- Different enrichment grades:
• Reactors: ~3–5 % ^{235}\text{U} ("low enriched").
• Weapons: >90 % ^{235}\text{U} ("highly enriched"). - Time scale matters: bombs must assemble super-critical mass faster than neutron generation; reactors purposely keep chain reaction slow and controlled.
Nuclear Reactors – Principles & Components
- Definition: Device sustaining a controlled chain reaction; heat → boil water → mechanical/electric power.
- Key distinction from bombs:
• Reactors use thermal (slow) neutrons; bombs rely on fast neutrons.
• Excess reactivity controlled with moderators, control rods, coolant. - Major parts:
• Fuel rods (usually \text{UO}_2 pellets, ~3–5 % ^{235}\text{U}).
• Moderator (light water, heavy water, graphite) reduces neutron speed via elastic collisions.
• Control rods (boron, cadmium, hafnium) absorb neutrons to throttle reaction.
• Coolant loop extracts heat; produces steam for turbines. - Cherenkov radiation: blue glow when charged particles (β electrons) outrun local light speed in water.
- Breeder reactors: Design converts fertile ^{238}\text{U} or ^{232}\text{Th} into fissile ^{239}\text{Pu} or ^{233}\text{U}; can generate more fuel than consumed.
- Generation IV concepts (e.g., lead-cooled fast reactors) rely on passive convection cooling for added safety.
Reactor Accidents & Lessons
- Three Mile Island (1979, USA):
• Cost-cutting → loss of secondary loop flow → primary loop overheated → partial core melt.
• Containment held; minimal radiation release.
• Lesson: importance of redundant cooling & transparent regulation. - Chernobyl (1986, USSR):
• Deliberate power-down test; low water flow + positive void coefficient.
• Graphite-tipped control rods displaced neutron-absorbing water, spiked reactivity.
• Steam explosion & graphite fire → wide radioactive release.
• Lesson: negative feedback & robust containment non-negotiable. - Fukushima Daiichi (2011, Japan):
• 9.0 earthquake + tsunami disabled grid and backup diesel generators (placed behind seawall).
• Loss of coolant → hydrogen buildup → four building explosions; significant release.
• Different failure mode vs. Chernobyl (no prompt criticality, but cooling failure).
Nuclear Waste Management – Yucca Mountain
- High-level waste remains radioactive 10³–10⁵ years.
- Proposed deep-geologic repository: Yucca Mountain, Nevada.
• ~300 m below surface, above water table.
• Access ramps & tunnels isolate canisters. - Political, ethical, and logistical challenges: long-term stewardship, intergenerational equity, security.
Fusion Power – Stellar, Tokamak, Laser & Muon Catalysis
- Fusion = combining light nuclei (e.g., D + T) → heavier nucleus + energy (via mass defect).
- Occurs naturally in stars:
• Hydrogen burning in sun → helium + photons → supports stellar radiation pressure.
• Larger stars produce heavier elements up to Fe, supernovae for elements beyond. - Tokamak magnetic confinement:
• Donut-shaped torus; toroidal + poloidal magnetic fields confine high-temperature (~10⁸ K) plasma.
• ITER (France) largest ongoing experiment. - Inertial confinement (laser) fusion:
• Symmetric laser pulses compress pellet to high density/temperature before it disassembles.
• National Ignition Facility (NIF) achieved > kilojoule-scale target energies. - Muon-catalyzed (cold) fusion:
• Muon replaces electron, shrinking D-T molecule → quantum tunneling allows fusion at low temp.
• Challenge: each muon must catalyze many fusions (>200) to offset production energy; ~1 % of muons “stick” to α, halting cycle → not yet practical.
Chapter Takeaways
- Chain reactions underpin phenomena from fetal growth to nuclear weapons.
- Exponential doubling 2^N yields rapid escalation; control mechanisms differentiate benign from catastrophic outcomes.
- Fission bombs need super-critical mass & microsecond assembly; critical mass ≈15 kg ^{235}\text{U}, 5 kg ^{239}\text{Pu}.
- Thermonuclear bombs dwarf fission devices using staged D-T fusion.
- Reactors harness slow-neutron fission for power; cannot explode like bombs but pose meltdown & waste challenges.
- Accidents (TMI, Chernobyl, Fukushima) illustrate diverse failure paths; robust safety culture essential.
- Future solutions: breeder & Gen-IV designs, effective waste repositories, and ultimately controlled fusion to emulate the sun’s power with minimal long-lived waste.