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Nuclear Decay and Radioactivity: Structure, Stability, and Decay Processes

스터디 가이드 - 스마트 노트

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Nuclear Decay

Introduction

Nuclear decay refers to the spontaneous transformation of an unstable atomic nucleus into a more stable one, accompanied by the emission of particles or electromagnetic radiation. This process is fundamental to understanding nuclear physics and radioactivity.

Describing the Nucleus

Constituents of the Nucleus

  • Protons: Positively charged particles with charge +e and mass kg.

  • Neutrons: Electrically neutral particles with mass kg.

  • Protons and neutrons are collectively called nucleons.

Nuclear Notation

  • Nuclei are represented as , where:

    • = chemical symbol (e.g., H, He, N)

    • = atomic number (number of protons)

    • = mass number (number of protons + neutrons)

Periodic Table and Atomic Structure

The periodic table organizes elements by increasing atomic number. Each element's identity is determined by its number of protons ().

Mass-Energy Equivalence

  • Einstein's equation:

  • is the rest energy of a particle, representing the energy due to its mass alone.

  • Mass and energy are interchangeable, provided total energy is conserved.

  • Mass is not strictly conserved; it can be converted to energy and vice versa.

Common Units of Mass

  • Atomic mass unit (u):

  • By convention, C has a mass of exactly 12 u.

  • MeV/:

  • Rest mass energy:

Particle

kg

u

MeV/

Proton

1.67262 × 10−27

1.00727

938.27

Neutron

1.67493 × 10−27

1.00866

939.57

Electron

9.10939 × 10−31

0.0005486

0.511

Nuclear Structure

  • Protons repel each other due to electrostatic (Coulomb) force.

  • Strong nuclear force: Attractive force between nucleons, much stronger than electrostatic repulsion but only effective at very short ranges (≈ m).

Nuclear Stability

  • Stable nuclei cluster near the line of stability (N ≈ Z for light elements).

  • No stable nuclei exist for (bismuth).

  • As increases, more neutrons are needed for stability.

Radioactivity

  • Unstable nuclei spontaneously emit particles or photons to become more stable.

  • Radioactive decay: Spontaneous emission of particles or high-energy photons from unstable nuclei.

Radiation

Identification

Charge

Stopped by

Alpha,

He nucleus

+2e

Sheet of paper

Beta,

Electron or positron

±e

Few mm of aluminum

Gamma,

High-energy photon

0

Many cm of lead

The Shell Model

  • Proposed by Maria Goeppert-Mayer (1949).

  • Each nucleon moves independently in an average potential due to the strong force from all other nucleons.

  • Energy levels (shells) exist for protons and neutrons, similar to electron shells in atoms.

Potential Energy Wells

  • Neutron potential well depth: ≈ 50 MeV for all nuclei.

  • Proton potential well is "lifted" by electrostatic repulsion, especially for high-Z nuclei.

Low-Z Nuclei

  • Energy levels for neutrons and protons are nearly identical for .

  • Example: C has closed n=2 shells for both protons and neutrons (6 each).

  • For N and B, the extra nucleon occupies the next available shell, leading to beta decay for increased stability.

Beta Decay

  • Two types: Beta-minus () and Beta-plus () decay.

  • Beta-minus: Neutron transforms into a proton, emitting an electron and an antineutrino.

  • Beta-plus: Proton transforms into a neutron, emitting a positron and a neutrino.

  • Neutrinos are emitted to conserve momentum and energy.

General equations:

  • Beta-minus:

  • Beta-plus:

High-Z Nuclei and Alpha Decay

  • High-Z nuclei have higher proton potential energy due to electrostatic repulsion.

  • When too many nucleons are present, the nucleus may eject an alpha particle (He nucleus) to become more stable.

  • Alpha decay is a quantum mechanical tunneling process.

Alpha decay equation:

Energy released:

Decay Series

  • Some decay products are themselves radioactive, leading to a decay series until a stable isotope is reached.

  • Multiple decay paths may exist.

Excited Nuclei

  • Radioactive decay often leaves the nucleus in an excited state.

  • Stability is achieved by emitting a high-energy photon (gamma decay).

  • Typical half-life of excited nuclear state: s.

Decay Rate and Activity

Decay Rate (r)

  • Probability per second that a nucleus will decay.

  • Example: If Hz, there is a 10% chance of decay per second.

Activity (R)

  • Number of decays per second in a sample.

Exponential Decay Law

  • The number of undecayed nuclei at time :

  • = initial number of nuclei

  • = decay rate

Half-Life ()

  • The time required for half the nuclei in a sample to decay.

  • Relationship to decay rate:

Alternative form for number of nuclei remaining:

Summary Table: Types of Radioactive Decay

Decay Type

Process

Particles Emitted

Example

Alpha ()

Loss of 2 protons, 2 neutrons

He nucleus

U Th + He

Beta-minus ()

Neutron proton

Electron, antineutrino

C N + +

Beta-plus ()

Proton neutron

Positron, neutrino

C B + +

Gamma ()

De-excitation of nucleus

Photon

Co* Co +

Applications and Examples

  • Medical Imaging: Use of isotopes like I in nuclear medicine.

  • Radiocarbon Dating: C decay used to date archaeological samples.

  • Nuclear Power: Controlled fission reactions in reactors.

Additional info: The notes also include worked example questions and data tables for practice, as well as references to textbook appendices for nuclear data.

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