Nuclear Reactions & Radioactive Decay – Comprehensive Study Notes
Binding Energy, Stability & General Features of Nuclear Reactions
- Binding-energy curve
- Binding energy per nucleon peaks for intermediate-mass nuclei (around Fe, Ni).
- ⟹ Fusing very light nuclei or fissioning very heavy nuclei moves products toward this maximum and releases large energy (mass defect → E=mc^{2}).
- Isotopic (nuclide) notation: ^{A}_{Z}X
- Z = atomic number = # protons.
- A = mass number = # protons + neutrons (nucleons).
- Conservation rules when writing/ balancing nuclear equations
- Total A on reactant side = total A on product side.
- Total Z on reactant side = total Z on product side.
- Energy, momentum & lepton number also conserved (latter omitted on MCAT except for noting antineutrino/ neutrino).
Fusion
- Definition: Combination of two (or more) light nuclei → heavier nucleus.
- Stellar example (proton–proton chain simplified):
4\,^{1}{1}H \;\rightarrow\;^{4}{2}He + 2e^{+}+2\nu_{e}+\text{energy}
- Sun outputs 3.85\times10^{26}\ \text{J·s}^{-1} (≈ 385 YW).
- Energy corresponds to small mass defect: missing mass converted to radiant energy.
- Terrestrial research
- Magnetic/ inertial confinement reactors (ITER, NIF) attempt ^{2}{1}H+^{3}{1}H or ^{2}{1}H+^{2}{1}H.
- Text’s given prototype: deuterium + lithium reactions inside experimental fusion power plants.
Fission
- Definition: Splitting of a heavy nucleus → two (or more) lighter nuclei + free neutrons + energy.
- Spontaneous fission rare (large Coulomb barrier); induced fission via absorption of low-energy (thermal) neutron practical.
- Chain reaction concept
- If each fission releases ≥ 1 extra neutron capable of causing another fission, a self-sustaining chain can occur.
- Controlled in reactors (moderator, control rods); uncontrolled in weapons.
- Classical MCAT example
- Capture: ^{235}{92}U + ^{1}{0}n \;\rightarrow\;^{236}_{92}U^{*} (excited).
- Fission products: ^{236}{92}U^{*}\;\rightarrow\;^{140}{54}Xe + ^{94}{38}Sr + x\,^{1}{0}n.
- Balancing A: 236-140-94 = 2 ⇒ x=2 neutrons.
- Balancing Z: 92-54-38=0 ✔️
- Released neutrons propagate the chain.
Radioactive Decay Overview
- Natural, spontaneous transmutation accompanied by emission of characteristic particles/ photons.
- MCAT problem types:
- Arithmetic of balancing nuclear symbols.
- Half-life calculations.
- Exponential-decay constant usage.
Alpha ( \alpha ) Decay
- Emission of an alpha particle ^{4}{2}\alpha \,(^{4}{2}He^{2+}).
- Daughter: Z{\text{daughter}} = Z{\text{parent}}-2; A{\text{daughter}} = A{\text{parent}}-4.
- Low penetration (stopped by few cm air / paper / skin).
- Example balance:
^{238}{92}U \;\rightarrow\;^{234}{90}Th + ^{4}_{2}\alpha.
Beta-Minus ( \beta^{-} ) Decay
- A neutron → proton + e^{-} + \bar{\nu}_{e}.
- Emitted particle: ^{0}_{-1}\beta^{-} (electron).
- Daughter: Z+1, A unchanged.
- Example: ^{146}{61}Pm \;\rightarrow\;^{146}{62}Sm + ^{0}_{-1}\beta^{-}.
Beta-Plus / Positron ( \beta^{+} ) Decay
- A proton → neutron + e^{+} + \nu_{e}.
- Emitted particle: ^{0}_{+1}\beta^{+}.
- Daughter: Z-1, A unchanged.
- Sample equation form: ^{A}{Z}X \;\rightarrow\;^{A}{Z-1}Y + ^{0}_{+1}\beta^{+}.
Gamma ( \gamma ) Emission
- High-energy photon (\gamma) emitted when nucleus transitions from excited ( * ) to lower energy.
- No change in A or Z.
- Notation: ^{A}{Z}X^{*} \;\rightarrow\;^{A}{Z}X + \gamma.
- Highly penetrating; requires dense shielding (lead, concrete).
Electron Capture (EC)
- Inner orbital electron captured by nucleus: p+e^{-}\rightarrow n+\nu_{e}.
- Equation: ^{A}{Z}X + e^{-} \;\rightarrow\;^{A}{Z-1}Y.
- Mass number same; atomic number decreases by 1.
- Often competes with \beta^{+} decay; thought of as its reverse.
Worked Decay-Chain Puzzle (combined modes)
- Given final ^{241}_{95}Am after: \alpha decay ← \beta^{+} decay ← \gamma emission.
- Last (\alpha): ^{245}{97}Bk \;\rightarrow\;^{241}{95}Am + ^{4}_{2}\alpha.
- Prior (\beta^{+}): ^{245}{98}Cf \;\rightarrow\;^{245}{97}Bk + ^{0}_{+1}\beta^{+}.
- First (\gamma): ^{245}{98}Cf^{*} \;\rightarrow\;^{245}{98}Cf + \gamma.
- Starting excited nucleus: ^{245}_{98}Cf^{*}.
Half-Life \bigl(t_{1/2}\bigr)
- Definition: Time required for ½ of initial radioactive nuclei to decay.
- After n half-lives, fraction remaining = (\tfrac{1}{2})^{n}.
- Example: t_{1/2}=4\,\text{yr}. After 12\,\text{yr}=3 half-lives ⇒ remaining fraction (\tfrac{1}{2})^{3}=\tfrac{1}{8}.
Exponential Decay Mathematics
- Differential form: \frac{dN}{dt} = -\lambda N.
- Solution: N(t)=N_{0}\,e^{-\lambda t}.
- Relation to half-life: \lambda = \frac{\ln 2}{t{1/2}} = \frac{0.693}{t{1/2}}.
- Sample calculation (transcript example):
- N_{0}=2\,\text{mol}, \lambda=2\,\text{h}^{-1}, t=0.75\,\text{h}.
- N = 2\,\text{mol}\,e^{-2(0.75)} = 2\,\text{mol}\,e^{-1.5} \approx 2\,\text{mol}\times0.22 = 0.44\,\text{mol}.
- Nuclei count: 0.44\,\text{mol}\times6.02\times10^{23}\,\frac{\text{nuclei}}{\text{mol}} \approx 2.64\times10^{23}\, nuclei remain.
Practical, Ethical & Real-World Connections
- Energy production
- Controlled fission supplies ≈ 10 % of global electricity; challenges: waste management, meltdown risk.
- Fusion promises abundant, cleaner energy; still net-negative today (2024).
- Medical imaging/ therapy
- \gamma emitters in PET/ SPECT; \beta^{+} tracers; radiotherapy uses \beta^{-} and \gamma.
- Astrophysics & cosmology
- Stellar nucleosynthesis, supernovae explain elemental abundances.
- Ethical considerations
- Nuclear weapons proliferation, accidents (Chernobyl, Fukushima), long-lived waste necessitate stringent regulation & international policy.
Quick MCAT Strategy Reminders
- Translate words ⟶ nuclide symbols; immediately check A & Z balance.
- Recognize particle symbols: ^{1}{0}n,\ ^{0}{-1}e,\ ^{0}{+1}e,\ ^{4}{2}\alpha,\ \gamma.
- For half-life mental math: set up powers of \tfrac{1}{2}; memorize \ln 2\approx0.693.
- Chain reactions: watch for extra neutrons (fission) or missing ones (fusion) to infer net effect.
- Keep units straight: J, eV (1 eV = 1.6\times10^{-19}\,\text{J}), W (J·s⁻¹), mol, nuclei.