IP Physics Notes (Upper Secondary, Year 3-4): 17) Radioactivity
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Quick recap -- Unstable nuclei shed energy by emitting alpha, beta, or gamma radiation. Identify the emission, update the nuclide notation, and use half-life reasoning to track activity changes.
Rutherford Scattering Recap
- Most alpha particles passed straight through gold foil -> atoms mostly empty space.
- Some deflected at large angles -> positive charge concentrated in tiny nucleus.
- A few rebounded -> nucleus is dense and carries most mass.
- Led to nuclear model: central nucleus (protons + neutrons) with orbiting electrons.
Nuclear Notation & Isotopes
- Nuclide represented as \( ^A_Z \text{X} \) where \( A \) is nucleon number, \( Z \) proton number.
- Isotopes share \( Z \) but have different neutron counts (different \( A \)).
- Proton number defines element; neutron-proton balance determines stability.
Types of Radioactive Emission
Radiation | Nature | Charge | Mass (amu) | Ionising power | Penetration |
Alpha (\( \alpha \)) | Helium nucleus (\( ^4_2 \text{He} \)) | +2 | 4 | Very strong | Stopped by paper / few cm air |
Beta (\( \beta^- \)) | High-speed electron (\( e^- \)) | -1 | 0 | Moderate | Stopped by few mm aluminium |
Gamma (\( \gamma \)) | EM wave | 0 | 0 | Weak | Requires thick lead/concrete |
Nuclear Equations
- Alpha decay \( \alpha\) or \(\text{He}^{2+}\): \[ ^A_Z \text{X} \to \space ^{A-4}_{Z-2} \text{Y} + \space ^4_2 \text{He} \]
- Beta decay \(\beta\) or \(\text{e}^-\):
\[ \begin{aligned} \text{neutron } n &\to& \text{proton } p^+ &\space&+&\space& \text{electron } e^- &\space&+&\space& \text{antineutrino } \overline{\nu} \\ ^A_Z \text{X} &\to& ^A_{Z+1} \text{Y} &\space&+&\space& ^0_{-1} \beta &\space&+&\space& \overline{\nu} \end{aligned} \] - Gamma emission accompanies other decays; no change to \( A \) or \( Z \); nucleus transitions to lower energy state.
Half-Life & Activity
- Half-life \( T_{1/2} \): time for activity or number of undecayed nuclei to halve.
- After \( n \) half-lives: remaining fraction \( = \left( \frac{1}{2} \right)^n \).
- Activity \( A \) (decays per second) proportional to number of undecayed nuclei.
Worked Example: Half-Life Count
A sample starts with activity \( \pu{6400 Bq} \). If half-life is \( \pu{12 h} \), find activity after \( \pu{36 h} \).
\[ 36 h = 3 \times 12 h \Rightarrow n = 3 \text{ half-lives}.\quad A = 6400 \left( \dfrac{1}{2} \right)^3 = \pu{800 Bq}. \]
Detecting Radiation
- Geiger-Mller tube: ionising radiation makes gas conductive; pulses counted.
- Photographic film: darkens under exposure.
- Scintillation detectors: light flashes converted to electrical signals.
- Always subtract background count when analysing data.
Applications & Risks
- Medical tracers (short half-life beta/gamma emitters).
- Radiotherapy (gamma/x-rays) for tumour destruction.
- Industrial thickness control (beta sources), smoke detectors (alpha sources).
- Hazards: ionisation of living tissue causing burns, cancer, or genetic damage.
- Safety: shielding, distance, minimised exposure time, proper storage, monitoring badges.
Key Takeaways
- Use nuclide notation carefully when balancing decay equations.
- Half-life problems often hinge on counting discrete halving steps; convert times accordingly.
- Gamma accompanies other emissions to shed excess energy; it doesn't alter \( A \) or \( Z \).
- Always mention safety protocols when discussing uses of radioactive sources.