Atomic Particles, Radiation & Nuclear Reactions – Comprehensive Study Notes

Major Atomic Particles – Quick Review

  • Three fundamental particles discussed:
    • Proton (p⁺)
    • Neutron (n⁰)
    • Electron (e⁻)
  • Everything that follows in the lecture is built on these three entities.

Beyond the Big Three – Hadrons, Leptons, Baryons, Quarks, Gluons

  • Two grand families (test will expect only definitions):
    • Hadrons (“heavy”)
    • Composite particles made of quarks.
    • Sub-classes: baryons (e.g.
      protons, neutrons – 3 quarks) & mesons (quark + antiquark).
    • Leptons (“light/elementary”)
    • Cannot be broken down further in the Standard Model.
    • Includes electrons, muons, tau, neutrinos.
  • Gluons
    • Exchange (force-carrier) particles that “glue” quarks together via the strong force.
    • Instructor anecdote: the whimsical name sparked a class contest to invent fake particles (e.g. “Pikachuon,” “Gokuon”) – these are fictional.
  • Take-away for exam: know the definitions of hadron, lepton, baryon, quark, gluon; no deeper math required.

Core Properties Table (copy-worthy)

ParticleApprox. Mass (AMU)Relative ChargeNuclear Location
Protonslightly < 1\text{ AMU}+1Inside nucleus
Neutron1\text{ AMU}0Inside nucleus
Electron\dfrac{1}{1800}\text{ AMU} (≈0.00055 AMU)-1Not in nucleus (orbitals/energy levels; Ch 5)
  • Extra numeric tidbits:
    • m{\text{neutron}} \approx m{\text{proton}} + m_{\text{electron}} (by ~0.1%)
    • 1.6\times10^{-19}\,\text{C} absolute charge → simplified to +1, –1, 0 for chem notation.

Forces Operating Inside the Nucleus

  • Electrostatic (Coulombic) Repulsion: F \propto \dfrac{q1q2}{r^2} — like charges repel (proton ↔ proton).
  • Strong Nuclear Force (Binding Force):
    • Short-range, ~10^{-15}\,\text{m}.
    • Acts between p–p, n–n, p–n alike; always attractive.
    • No everyday analogue – unique to the nucleus.
  • Role of Neutrons
    • Insert spacing (increase r) between protons → weaken Coulomb term while still participating in the strong force.
    • Too few neutrons → electrostatic repulsion wins (instability).
    • Too many neutrons → nucleus becomes overly massive; strong force cannot bind the excess → instability.

Radiation & the Drive Toward Stability

  • Nature favors exothermic, lower-energy states.
  • High-mass or unbalanced nuclei shed excess energy via radiation (particles/photons) until a stable n⁄p ratio is reached.
  • “Heavy” = large Z (protons) and large N (neutrons).

Four Major Radiation Types (plus X-rays)

1. Alpha (α) Radiation

  • Notation in text: α ; in equations: ^{4}_{2}He (helium nucleus).
  • Properties
    • Mass = 4 AMU, charge = +2.
    • Low velocity ⇒ low KE despite high mass.
  • Penetration / Hazard
    • Stopped by paper/skin; dangerous only if ingested (food, lungs).

2. Beta (β⁻) Radiation

  • Neutron → proton + electron; electron ejected.
  • Equation notation: ^{0}_{-1}e or \beta.
  • Properties
    • Negligible mass, high velocity.
    • Charge = –1 ⇒ slowed by Coulomb attractions inside matter.
  • Penetration
    • Passes through paper/wood, stopped by thin metal (Al).

3. Gamma (γ) Rays

  • Pure electromagnetic energy, no mass, no charge.
  • Notation in equations: γ (no isotope numbers).
  • Very high E (higher than X-rays).
  • Penetration
    • Passes through most materials; attenuated only by dense lead or several cm of concrete.
    • Primary health risk: deep tissue ionization → leukemia/cancers (Hulk fiction vs. reality).

4. Neutron Emission (n)

  • Notation: ^{1}_{0}n.
  • High mass and high velocity; neutral → no Coulomb slowing.
  • Most penetrating / dangerous among listed particles.
  • Practical role: triggers chain reactions in fission bombs & reactors.

5. X-Rays (for completeness)

  • Same class as γ but lower energy; blocked by lead aprons in medical imaging.

Comparative Penetration Summary

RadiationMassChargeVelocityNet KEShielding
\alphaHigh+2LowModeratePaper/skin
\betaVery low–1HighModerateMetal foil
\gamma00cHigh (E = hν)Lead/concrete
n1 AMU0HighVery HighH-rich concrete, water, boron

Why Penetration Depends on KE and Charge

  • KE = \tfrac{1}{2}mv^{2} — needs both mass and velocity.
  • Charged particles lose KE via Coulombic interactions inside matter (ionization, excitation) → slow down.
  • Neutral particles or photons have no such losses, so travel farther.

Nuclear Reactions Overview

1. Fission ("decay" ≈ decomposition)

  • Large nucleus → smaller nuclei + particles + energy.
  • Often spontaneous for very heavy isotopes or induced by neutron capture.

2. Fusion (synthesis)

  • Small nuclei combine to form a larger one.
  • Powers stars; requires extreme T/P to overcome Coulomb barrier.

Balancing Nuclear Equations – Rules & Examples

  1. Conserve mass number (A) – sum of top numbers.
  2. Conserve atomic number (Z) – sum of bottom numbers (protons).
  3. Electrons are ignored (unless explicitly β in equation).

Simple Fusion Example


^{1}{1}H + ^{3}{1}H \;\longrightarrow\; ^{4}_{2}He

  • A: 1+3=4 ✓
  • Z: 1+1=2 ✓ (He)

Multi-step Fission/Decay Example

Given ^{238}_{92}U undergoes 2 α + 1 β⁻ decays, find product X.

Work:

  • Subtract two α: A:238-2\times4=230, Z:92-2\times2=88
  • Subtract one β⁻ (adds 1 to Z): Z=88+1=89
  • Result: ^{230}_{89}Ac (actinium-230).

Fusion Puzzle Example (class exercise)

"What must merge with ^{12}{6}C to form ^{25}{12}Mg?"

  • Need A: 25-12=13, Z: 12-6=6 ⇒ ^{13}_{6}C.

Average Atomic Mass – Weighted Mean of Isotopes

  • General formula (n isotopes):
    \text{Avg Mass}=\sum{i=1}^{n} \left(\text{abundance}i \times \text{mass}_i\right)
    (abundance expressed as decimal, not %).

Worked Carbon Example (lecture numbers)

  • Isotopes & abundances:
    • ^{12}C: 98.50 % (0.9850), mass = 11.998 AMU.
    • ^{14}C: 1.50 % (0.0150), mass = 13.987 AMU.
  • Calculation:
    0.9850\times11.998 + 0.0150\times13.987 = 11.82 + 0.2098 \approx 12.03\,\text{AMU}
  • Close to standard 12.011\,\text{AMU} (nat. abundances slightly different).
  • Sig-fig protocol: multiply – look at total sig figs; add – align decimal places.

Ethical, Practical & Real-World Implications

  • Radiation safety: alpha sources safe if sealed; beta/gamma require shielding; neutron/gamma relevant in nuclear reactors, space travel.
  • Medical imaging: X-ray vs. γ-ray exposure, lead aprons, dose limits.
  • Energy production vs. weapons: fission chain reactions, neutron moderation.
  • Climate relevance: fusion research (ITER) aims for cleaner energy.

Instructor Anecdotes & Helpful Reminders

  • You must memorize notation ^{4}{2}He, ^{0}{-1}e, ^{0}{0}\gamma, ^{1}{0}n for exam.
  • Copy the properties table verbatim; simplest way to recall p/n/e data.
  • Balancing nuclear equations is easier than redox: just add/subtract A & Z.
  • Electrons do “weird things” – detailed electron behavior postponed to Chapter 5.
  • Remember Dr. Checker’s maxim: “To prove something exists, you must first imagine it.” (Applies to theoretical physics & creative problem-solving.)