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Understanding Nuclear Chemistry and Radioactivity
Sep 5, 2024
Nuclear Chemistry and Radioactivity
Overview
Introduction to Nuclear Chemistry
Combined with chemical kinetics and atomic structure
Two parts of Nuclear Chemistry:
Theoretical part
Definitions: Radioactivity, radioactive disintegration series, stability of the nucleus
Related to atomic structure
Numerical part
First order kinetics of radioactive decay
Applications: Rock dating, carbon dating
Lecture Structure
3-4 initial lectures for 11th class students after atomic structure
2-3 later lectures after chemical kinetics
Key Concepts
Nuclear Chemistry
Nucleus as a 'black box'; primarily studied in physics
Research focused on understanding the nucleus: nucleons (neutrons and protons) distribution
Extranuclear chemistry vs. intranuclear chemistry
Radioactivity
Definition:
Spontaneous decay of unstable nuclei without external excitation
Emission of alpha, beta, and gamma rays
Unstable nuclei undergo nuclear decay spontaneously
Nuclear Stability
Stability of the nucleus:
Electronic repulsion reduced by the spread of electrons in large space
Nuclear forces: Operate at nuclear distances (around 10^-15 meters or femtometer)
Nuclear forces of attraction are stronger than electrostatic repulsion among protons
Evidence from alpha particle scattering experiment
Potential Energy vs Distance
Potential energy increases with distance due to columbic repulsion
At nuclear distances, attractive nuclear forces dominate
Attractive forces among protons and neutrons create stability
Yukawa's Meson Theory
Proposed in 1935 by Yukawa for nucleus stability
Rapid exchange of pi mesons between nucleons (protons and neutrons) leads to stability
Pi mesons: electrically neutral, positive, or negative
Heavier than electrons
Mass Defect and Binding Energy
Mass defect: Atoms are slightly lighter than the sum of their constituent particles
Example: Oxygen-16 atom has mass 15.99 amu vs. sum of 16.13 amu
Binding energy: Energy released when forming a nucleus from its nucleons
Calculated using Einstein's equation: E = ΔM * c²
1 amu mass loss corresponds to approximately 931.4 MeV energy released
Higher binding energy per nucleon = greater stability of the nucleus
Maximum binding energy per nucleon around mass number 60 (Iron)
Fusion and Fission
Light nuclei undergo fusion for stability
Heavy nuclei undergo fission to reach stable zones
Example: Fusion in stars, like the sun
Conclusion
Overview of nuclear stability, mass defect, and binding energy
Future discussions on magic numbers and related topics in next lectures
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