Modern Physics: Real-World Scenarios (6)

hard 2 min read

Question

A radioactive sample has a half-life of 20 days. Initially it has 4×10204 \times 10^{20} atoms. How many atoms remain after 60 days, and what is the activity at that moment?

Solution — Step by Step

60/20=360 / 20 = 3 half-lives. After each half-life, the number halves.

N=N0(12)3=N08N = N_0 \left(\frac{1}{2}\right)^3 = \frac{N_0}{8}

N=4×10208=5×1019 atomsN = \frac{4 \times 10^{20}}{8} = 5 \times 10^{19}\text{ atoms}

λ=ln2T1/2=0.69320×86400 s14.01×107 s1\lambda = \frac{\ln 2}{T_{1/2}} = \frac{0.693}{20 \times 86400}\text{ s}^{-1} \approx 4.01 \times 10^{-7}\text{ s}^{-1}

A=λN=4.01×107×5×10192.0×1013 BqA = \lambda N = 4.01 \times 10^{-7} \times 5 \times 10^{19} \approx 2.0 \times 10^{13}\text{ Bq}

Final answer: N=5×1019N = 5 \times 10^{19} atoms, A2.0×1013A \approx 2.0 \times 10^{13} Bq

Why This Works

Radioactive decay is a first-order process: the rate at which atoms decay is proportional to how many are left. This gives the exponential law N(t)=N0eλtN(t) = N_0 e^{-\lambda t}, equivalent to halving every T1/2=ln2/λT_{1/2} = \ln 2 / \lambda.

The activity (decays per second) is just λN\lambda N, so it shrinks by the same factor of 8 over 3 half-lives.

Alternative Method

For non-integer numbers of half-lives, use N=N0eλtN = N_0 e^{-\lambda t} directly. For integer multiples, the powers-of-2 trick is much faster.

Common Mistake

Students compute N=N0N0/8=7N0/8N = N_0 - N_0/8 = 7N_0/8, thinking “1/8 has decayed”. Wrong — 1/81/8 remains, 7/87/8 has decayed. Read the question carefully: “atoms remain” vs “atoms decayed” gives different answers.

Carbon dating uses this exact math with T1/2(C-14)=5730T_{1/2}(\text{C-14}) = 5730 years. NEET 2023 asked a 5730-year wood sample question — same powers-of-2 logic.

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