Lesson 5 of 15

Radioactive Decay Law

Radioactive Decay Law

In the previous lesson we derived the decay constant λ\lambda. Now we use it to track how a population of nuclei evolves over time.

Number of Nuclei Over Time

Solving dN/dt=λNdN/dt = -\lambda N gives:

N(t)=N0eλtN(t) = N_0 \, e^{-\lambda t}

where N0N_0 is the initial number of nuclei. Equivalently, using the half-life t1/2t_{1/2}:

N(t)=N0(12)t/t1/2N(t) = N_0 \left(\frac{1}{2}\right)^{t/t_{1/2}}

Fraction Remaining

The fraction of original nuclei still present:

N(t)N0=eλt\frac{N(t)}{N_0} = e^{-\lambda t}

After exactly one half-life: eλt1/2=eln2=0.5e^{-\lambda \cdot t_{1/2}} = e^{-\ln 2} = 0.5

After nn half-lives: (12)n\left(\frac{1}{2}\right)^n

Activity Over Time

The activity (decay rate) also follows exponential decay:

A(t)=λN(t)=λN0eλt=A0eλtA(t) = \lambda N(t) = \lambda N_0 \, e^{-\lambda t} = A_0 \, e^{-\lambda t}

where A0=λN0A_0 = \lambda N_0 is the initial activity in Becquerel (Bq).

Example: Carbon-14 Dating

C-14 has a half-life of 5730 years. A living organism maintains a constant C-14/C-12 ratio. After death, C-14 decays with no replenishment. Measuring the fraction remaining tells us the age:

t=1λln(NN0)t = -\frac{1}{\lambda} \ln\left(\frac{N}{N_0}\right)

After one half-life (5730 yr), exactly half the C-14 remains. After two half-lives (11460 yr), one quarter remains.

Your Task

Implement three functions. All constants must be defined inside each function.

  • nuclei_remaining(N0, lambda_s, t) — returns N0eλtN_0 \, e^{-\lambda t}
  • fraction_remaining(lambda_s, t) — returns eλte^{-\lambda t}
  • activity(N0, lambda_s, t) — returns λN0eλt\lambda N_0 \, e^{-\lambda t} in Bq
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