Nuclei Decomposition and Radioactivity Study Notes LEC14
Nuclei Decomposition Causes
Strong force holds nucleus particles together.
Neutrons stabilize the nucleus by adding to the strong force without repelling each other.
N/Z Ratio
Ratio of neutrons to protons indicates nucleus stability.
High N/Z ratio: neutrons convert to protons via beta decay.
Low N/Z ratio: protons convert to neutrons via positron emission/electron capture, or alpha decay.
Valley of Stability
Stable N/Z ratios:
Z = 1-20: N/Z ≈ 1
Z = 20-40: N/Z approaches 1.25
Z = 40-80: N/Z approaches 1.5
Z > 83: no stable nuclei.
Radioactive Decay Example
Mg-22 (Z = 12, N = 10, N/Z = 0.83): undergoes positron emission or electron capture due to low N/Z.
Magic Numbers
Stability is affected by even numbers of protons/neutrons.
Stable nuclei favor magic numbers: N or Z = 2, 8, 20, 28, 50, 82, 126.
Decay Series
A chain of radioactive nuclides until reaching a stable nuclide.
Determine stable nuclide by counting alpha and beta decays.
Detecting Radioactivity
Radioactive rays can expose film (film badge dosimeters).
Ionization detection by electroscope and Geiger-Müller counter.
Scintillation counters detect radiation via flashes of light.
Kinetics of Radioactive Decay
First-order kinetics: Rate = \frac{\Delta N}{\Delta t} = kN.
Each radionuclide has a specific half-life; shorter half-lives indicate faster decay.
Half-life formula: t_{\frac{1}{2}} = \frac{\ln 2}{k}.
Half-Lives of Various Nuclides
Th-232: 1.4 x 10^{10} yr (alpha decay)
U-238: 4.5 x 10^{9} yr (alpha decay)
C-14: 5730 yr (beta decay)
Rn-220: 55.6 sec (alpha decay).
Radiometric Dating
Measure parent radioactive isotopes versus stable daughter isotopes to determine age.
Example: U-238 to Pb-206 dating Earth’s age (4.0-4.5 billion yrs).
Radiocarbon Dating
C-14 decays with a half-life of 5730 yrs; produced at a steady rate.
Ratios of C-14/C-12 decrease post-mortem, allowing age estimation.
Effective for objects up to 50,000 years old.
Nonradioactive Nuclear Changes
Nuclear fission: large nucleus splits into smaller ones when hit by a neutron.
Nuclear fusion: small nuclei combine to form larger ones.
Both fission and fusion release significant energy, with fusion being more energy-efficient.