Radioactive Dating — Question 8

Section 42-6 · Physics pages 7106–7107

Question 8 Relative isotope uncertainty becomes an absolute age uncertainty An ideal radioactive clock has known half-life T = 5730 y and measured surviving fraction f = .250 ± .010, where the uncertainty is one standard deviation and is small enough for linear propagation. t/T1/2 f Schematic; labels, not drawing lengths, specify the data. (a) Derive the age uncertainty from t = −T ln f/ ln 2. (b) Find age and uncertainty, then determine the precision in f required for an age uncertainty of 100 y at the same fraction.
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Question 8 - Solution Relative isotope uncertainty becomes an absolute age uncertainty t/T1/2 f (a) Method and calculation dt df = − T f ln 2 ⇒σt = T ln 2 σf f . t = 11460 y, σt = 330.7 y . (b) Interpretation and further calculation σf = f(ln 2)σt/T. σf = .250(ln 2)(100)/5730 = .003024 . Physical check This uncertainty includes only the measured fraction. Half-life, calibration and contamination uncertainties would require additional terms or a fuller model.

Question 8

Relative isotope uncertainty becomes an absolute age uncertainty

An ideal radioactive clock has known half-life T=5730T=5730 y and measured surviving fraction f=.250±.010f=.250\pm.010, where the uncertainty is one standard deviation and is small enough for linear propagation.

Diagram shown in the original SVG worksheet.

  1. Derive the age uncertainty from t=−Tln⁡f/ln⁡2t=-T\ln f/\ln2.

  2. Find age and uncertainty, then determine the precision in f required for an age uncertainty of 100 y at the same fraction.

Question 8 - Solution

Relative isotope uncertainty becomes an absolute age uncertainty

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dtdf=−Tfln⁡2⇒σt=Tln⁡2σff.\frac{dt}{df}=-\frac{T}{f\ln2}\Rightarrow\boxed{\sigma_t=\frac{T}{\ln2}\frac{\sigma_f}{f}}.t=11460y,σt=330.7y.\boxed{t=11460\,\mathrm y,\quad\sigma_t=330.7\,\mathrm y}.

(b) Interpretation and further calculation

σf=f(ln⁡2)σt/T.\sigma_f=f(\ln2)\sigma_t/T.σf=.250(ln⁡2)(100)/5730=.003024.\boxed{\sigma_f=.250(\ln2)(100)/5730=.003024}.

Physical check

This uncertainty includes only the measured fraction. Half-life, calibration and contamination uncertainties would require additional terms or a fuller model.