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Chapter 34: Nuclear Fission and Fusion – Study Notes

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Chapter 34: Nuclear Fission and Fusion

Introduction

This chapter explores the fundamental processes of nuclear fission and nuclear fusion, their discovery, mechanisms, technological applications, and their significance in energy production and astrophysics. The chapter also discusses mass–energy equivalence and the challenges and prospects of harnessing nuclear energy.

Discovery of Nuclear Fission

Historical Background

  • 1934, Rome: Enrico Fermi and his team began bombarding uranium with neutrons, aiming to create transuranium elements.

  • 1935, Berlin: Lise Meitner and Otto Hahn started similar experiments, later joined by Otto Frisch for theoretical interpretation.

  • 1938: Discovery that neutron bombardment of uranium-235 produced elements chemically similar to barium, much lighter than uranium, leading to the realization that the uranium nucleus had split.

  • The process was named nuclear fission.

  • Meitner and Frisch provided the theoretical explanation, while Hahn published the experimental results.

Historical physicist in laboratoryHistorical physicist at deskHistorical chemist portrait

Key Insights

  • It was previously believed that nuclear changes occurred only in small steps.

  • The discovery of fission showed that a heavy nucleus could split into two lighter nuclei, releasing enormous energy.

Nuclear Fission: Mechanism and Energy Release

Forces in the Nucleus

  • The strong nuclear force holds nucleons (protons and neutrons) together at short distances.

  • If protons are separated enough, the electrical repulsion can overcome the strong force, causing the nucleus to split (fission).

Strong nuclear force vs electrical forceNuclear deformation and fission

Fission Reaction Example

  • A typical induced fission reaction for uranium-235:

Uranium-235 fission reaction diagram

Energy Release in Fission

  • Fragments are repelled at high speeds, carrying about 200 MeV of kinetic energy.

  • Some energy is released as kinetic energy of neutrons and gamma radiation.

  • Fission of uranium-235 releases about 200,000,000 eV per event, compared to 3–4 eV for a TNT molecule.

Chain Reaction

  • A chain reaction occurs when the neutrons produced by one fission event induce further fission events.

Chain reaction diagram

Critical Mass

  • Critical mass: The minimum mass of fissile material needed for a self-sustaining chain reaction.

  • Subcritical: Reaction fizzles out; Supercritical: Reaction grows explosively.

Critical mass and neutron escape

Isotopes and Fission

  • Not all uranium isotopes are fissile; U-235 is, but U-238 is not.

  • Most neutrons in natural uranium are absorbed by U-238, not causing fission.

U-235 and U-238 abundance

Harnessing Nuclear Fission Power

Reactors and Moderators

  • Reactors use moderators (like graphite) to slow down neutrons, increasing the probability of fission in U-235.

  • German scientists used heavy water, which was less effective and less available, contributing to the failure of their nuclear program.

Fission Bombs

  • Atomic bombs (e.g., Little Boy and Fat Man) used fission of uranium or plutonium.

  • Enrichment increases the percentage of U-235 for weapons or reactor fuel.

Fission bomb (Fat Man)Uranium enrichment process

Nuclear Fission Reactors

  • First reactor built under University of Chicago’s Stagg Field, supervised by Enrico Fermi.

  • Reactors generate heat to boil water, producing steam to drive turbines and generate electricity.

  • Key components: nuclear fuel, control rods, moderator, heat-extracting fluid.

Historical nuclear reactor settingNuclear reactor schematic

Reactor Safety and Accidents

  • Heat must be removed efficiently to prevent meltdown.

  • Major accidents: Chernobyl (1986), Fukushima (2011).

Containment building for nuclear reactor

Breeder Reactors

  • Breeder reactors convert U-238 into fissile Pu-239, which can be used as fuel.

Breeder reactor process

Pros and Cons of Fission Power

  • Benefits: Plentiful electricity, conserves fossil fuels, reduces CO2 emissions.

  • Drawbacks: Radioactive waste, risk of accidents, potential for weaponization.

Mass–Energy Equivalence

Einstein’s Equation

  • Mass is a form of potential energy, as described by Einstein’s equation:

  • During fission, the total mass of the products is less than the original nucleus; the difference is released as energy.

  • This mass difference is called the mass defect and is equivalent to the binding energy of the nucleus.

Mass defect illustration

Binding Energy and Mass per Nucleon

  • The binding energy is the energy required to separate a nucleus into its individual nucleons.

  • Mass per nucleon decreases as nucleons bind together, releasing energy.

Mass per nucleon plot

Energy Released in Fission

  • Fission of uranium-235 releases about 200 MeV per event, 7 million times more than a TNT molecule.

Nuclear Fusion

Fusion Process

  • Nuclear fusion: Two or more light nuclei combine to form a heavier nucleus, releasing energy.

  • Fusion converts a higher percentage of mass to energy than fission (up to 0.7%).

Nuclear fusion process

Conditions for Fusion

  • High temperatures are required to overcome the electrical repulsion between nuclei (thermonuclear fusion).

  • Occurs naturally in stars, including the Sun.

Fusion in stars

Nucleosynthesis

  • Big Bang nucleosynthesis: Formation of light elements (H, He, Li) in the early universe.

  • Stellar nucleosynthesis: Fusion in stars creates heavier elements up to iron.

  • Supernova nucleosynthesis: Creation of the heaviest elements during supernova explosions.

  • Cosmic ray spallation: High-energy cosmic rays break nuclei into lighter elements.

  • Neutron star mergers: Produce very heavy elements like gold and platinum.

Controlling Fusion

  • Fusion on Earth requires extremely high temperatures, achieved in hydrogen bombs using a fission trigger.

  • Fusion reactors (magnetic and inertial confinement) are under development but have not yet achieved net energy gain.

  • Fusion fuel (hydrogen) is abundant, and the main byproduct is nonradioactive helium.

Summary Table: Masses and Masses per Nucleon of Some Isotopes

Isotope

Symbol

Mass (amu)

Mass/Nucleon (amu)

Neutron

n

1.008665

1.008665

Hydrogen

^1H

1.007825

1.007825

Deuterium

^2H

2.01410

1.00705

Tritium

^3H

3.01605

1.00535

Helium-4

^4He

4.00260

1.00065

Carbon-12

^12C

12.00000

1.00000

Iron-56

^56Fe

55.93494

0.99884

Copper-63

^63Cu

62.92960

0.99888

Krypton-90

^90Kr

89.91951

0.99911

Barium-143

^143Ba

142.92065

0.99945

Uranium-235

^235U

235.04393

1.00109

Conclusion

Nuclear fission and fusion are powerful processes that release vast amounts of energy by converting mass into energy, as described by Einstein’s equation. Fission is currently used in nuclear reactors and weapons, while fusion powers stars and holds promise for future energy production. Understanding these processes is crucial for both technological advancement and addressing global energy needs.

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