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QLDPhysicsSyllabus dot point

Topic 2: Ionising radiation and nuclear reactions

Solve problems involving the exponential decay of radioactive nuclides, half-life and decay constant, and apply to radiometric dating and medical applications

A focused answer to the QCE Physics Unit 1 dot point on half-life and radioactive decay. Applies N=N0(1/2)t/T1/2N = N_0 (1/2)^{t/T_{1/2}} and the decay constant λ=ln2/T1/2\lambda = \ln 2 / T_{1/2}, walks through radiometric dating (carbon-14) and medical applications (technetium-99m), and works the QCAA-style number-of-half-lives problem.

Generated by Claude Opus 4.88 min answer

Reviewed by: AI editorial process; not yet individually human-reviewed

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  1. What this dot point is asking
  2. Exponential decay
  3. Half-life
  4. Radiometric dating
  5. Nuclear medicine
  6. How this appears in IA1 and EA
  7. Examples in context
  8. Try this

What this dot point is asking

QCAA wants you to apply the exponential decay law to find the number of nuclei remaining (or activity) at a given time, and to convert between half-life and decay constant. The dot point also covers two big applications: radiometric dating and nuclear medicine.

Exponential decay

Radioactive decay is a first-order process: each nucleus has a constant probability per unit time of decaying, independent of how old it is. This means the population follows an exponential curve:

N(t)=N0eλtN(t) = N_0 e^{-\lambda t}

where N0N_0 is the number at t=0t = 0 and λ\lambda is the decay constant (s1^{-1}). The activity (decays per second) is

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

SI unit of activity: becquerel (Bq, 11 Bq = 11 decay s1^{-1}).

Half-life

The half-life T1/2T_{1/2} is the time for half the nuclei in a sample to decay. From the exponential law:

T1/2=ln2λ0.693λT_{1/2} = \frac{\ln 2}{\lambda} \approx \frac{0.693}{\lambda}

For integer numbers of half-lives, use the convenient form:

N=N0(12)t/T1/2N = N_0 \left(\tfrac{1}{2}\right)^{t / T_{1/2}}

After 11 half-life: 1/21/2 remains. After 22: 1/41/4. After nn: (1/2)n(1/2)^n.

Radiometric dating

Carbon-14 (T1/2=5730T_{1/2} = 5730 years) is continuously produced in the upper atmosphere and absorbed by living things in equilibrium with atmospheric levels. When an organism dies, intake stops and the C-14 decays. Measuring the remaining C-14 fraction gives the time since death.

Uranium-238 (T1/2=4.5×109T_{1/2} = 4.5 \times 10^9 years) and other long-lived isotopes are used to date rocks.

Nuclear medicine

Technetium-99m (T1/2=6T_{1/2} = 6 hours) is the most-used medical radionuclide. It emits a gamma photon that an imaging camera detects, and its short half-life means most of the dose has decayed away by the next day. Iodine-131 (T1/2=8T_{1/2} = 8 days) is used to treat thyroid disorders because it concentrates in the thyroid gland.

How this appears in IA1 and EA

IA1 data test
Often a decay curve to read (activity vs time), with a half-life to extract and a future activity to predict.
EA Paper 1
Multiple choice on (1/2)n(1/2)^n for integer nn.
EA Paper 2
A two-part calculation: convert T1/2T_{1/2} to λ\lambda, then find activity or number remaining at a non-integer number of half-lives using the exponential formula.

Examples in context

Example 1. The Royal Brisbane and Women's Hospital uses technetium-99m for bone scans. Its half-life is 6.0 h6.0 \text{ h}. A patient is injected at 08000800 with 800 MBq800 \text{ MBq}; by the scanner at 11001100 (3.0 h3.0 \text{ h} later, t/T1/2=0.5t/T_{1/2} = 0.5), activity is A=A0(1/2)0.5=800×0.707=566 MBqA = A_0 (1/2)^{0.5} = 800 \times 0.707 = 566 \text{ MBq}. By 20002000 that evening (t/T1/2=2t/T_{1/2} = 2) the activity has dropped to A0/4=200 MBqA_0/4 = 200 \text{ MBq}, well below detection threshold. Decay-constant accounting λ=ln2/T1/2\lambda = \ln 2 / T_{1/2} underpins the dosing-and-schedule pharmacy software used statewide.

Example 2. Carbon-14 dating of charcoal from a Mt Cotton archaeological site yields a 14C/12C^{14}\text{C}/^{12}\text{C} ratio that is 0.300.30 of modern. With T1/2=5730 yearsT_{1/2} = 5730 \text{ years}, N/N0=0.30N/N_0 = 0.30 gives t=T1/2ln(0.30)/ln2=5730×1.737=9.95×103 yearst = -T_{1/2} \ln(0.30) / \ln 2 = 5730 \times 1.737 = 9.95 \times 10^3 \text{ years}. QCAA EA Unit 1 thematic items often pair such datasets with a brief on the assumptions (constant atmospheric ratio, closed system since burial), allowing a top-band candidate to flag where uncertainty in λ\lambda propagates into the inferred date.

Try this

Q1. State the half-life relationship for the number of nuclei, and find N/N0N/N_0 after three half-lives. [2 marks]

  • Cue. N=N0(1/2)t/T1/2N = N_0 (1/2)^{t/T_{1/2}}; after three half-lives, N/N0=1/8N/N_0 = 1/8.

Q2. A sample of iodine-131 (T1/2=8.0 daysT_{1/2} = 8.0 \text{ days}) has an initial activity of 480 MBq480 \text{ MBq}. Calculate the activity after 24 days24 \text{ days} and the decay constant λ\lambda. [3 marks]

  • Cue. t/T1/2=3t/T_{1/2} = 3, so A=60 MBqA = 60 \text{ MBq}; λ=ln2/(8×86400)=1.00×106 s1\lambda = \ln 2 / (8 \times 86400) = 1.00 \times 10^{-6} \text{ s}^{-1}.

Q3. A bone-scan dose contains 30 MBq30 \text{ MBq} of technetium-99m (T1/2=6.0 hT_{1/2} = 6.0 \text{ h}). (a) Calculate the activity after 18 h18 \text{ h}. (b) Determine the time for the activity to fall to 1.0 MBq1.0 \text{ MBq}. (c) Justify why short-half-life isotopes are preferred for diagnostic imaging. [2+3+2 marks; ISMG: Analysis and interpretation, Evaluation]

  • Cue. (a) 3.75 MBq3.75 \text{ MBq}; (b) t=T1/2log2(30)=29.4 ht = T_{1/2} \log_2(30) = 29.4 \text{ h}; (c) lower lifetime patient dose plus rapid clearance.

Exam-style practice questions

Practice questions written in the style of QCAA exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

Year 11 SAC4 marksA sample contains 8.0×10128.0 \times 10^{12} atoms of cobalt-60, with half-life 5.275.27 years. (a) How many atoms remain after 21.0821.08 years? (b) Calculate the decay constant in s1^{-1}.
Show worked answer →

(a) Number of atoms after 21.0821.08 years.

Number of half-lives: n=21.08/5.27=4.0n = 21.08 / 5.27 = 4.0.

N=N0(1/2)n=(8.0×1012)(1/2)4=(8.0×1012)/16=5.0×1011N = N_0 (1/2)^n = (8.0 \times 10^{12}) (1/2)^4 = (8.0 \times 10^{12})/16 = 5.0 \times 10^{11} atoms.

(b) Decay constant.

T1/2=5.27T_{1/2} = 5.27 years =5.27×365.25×24×3600=1.66×108= 5.27 \times 365.25 \times 24 \times 3600 = 1.66 \times 10^8 s.

λ=ln2/T1/2=0.693/(1.66×108)=4.17×109\lambda = \ln 2 / T_{1/2} = 0.693 / (1.66 \times 10^8) = 4.17 \times 10^{-9} s1^{-1}.

Markers reward the use of (1/2)n(1/2)^n with integer nn, conversion of years to seconds, and the formula λ=ln2/T1/2\lambda = \ln 2 / T_{1/2}.

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