Nuclear Fission: The Basic Process — Question 10

Section 43-1 · Physics pages 7170–7171

Question 10 Calorimetry and event counts give an experimental energy per fission A detector infers N = (2.00 ± .04) × 109 events in a pulse. A separate calorimeter measures deposited energy E = .0600 ± .0018 J. The stated errors are independent standard uncertainties. Use 1 MeV = 1.602 × 10−13 J. event counter: N calorimeter: E q = E/N Schematic; labels, not drawing lengths, specify the data. (a) Infer the deposited energy per fission and its propagated standard uncertainty. (b) A model predicts 190 MeV deposited per fission with negligible uncertainty. Quantify the discrepancy in standard deviations.
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Question 10 - Solution Calorimetry and event counts give an experimental energy per fission event counter: N calorimeter: E q = E/N (a) Method and calculation q = E/N = 3.00 × 10−11 J = 187.266 MeV . σq q = √ (.0018/.0600)2 + (.04/2.00)2 = .036056. (b) Interpretation and further calculation σq = 6.752 MeV, q = (187.3 ± 6.8) MeV . z = 187.266 −190 6.752 = −.405 consistent at this precision. Physical check Shared calibration errors would require a covariance term. A measurement of deposited energy need not equal the full nuclear Q value.

Question 10

Calorimetry and event counts give an experimental energy per fission

A detector infers N=(2.00±.04)×109N=(2.00\pm.04)\times10^9 events in a pulse. A separate calorimeter measures deposited energy E=.0600±.0018E=.0600\pm.0018 J. The stated errors are independent standard uncertainties. Use 1MeV=1.602×10−131\,\mathrm{MeV}=1.602\times10^{-13} J.

Diagram shown in the original SVG worksheet.

  1. Infer the deposited energy per fission and its propagated standard uncertainty.

  2. A model predicts 190 MeV deposited per fission with negligible uncertainty. Quantify the discrepancy in standard deviations.

Question 10 - Solution

Calorimetry and event counts give an experimental energy per fission

Diagram shown in the original SVG worksheet.

(a) Method and calculation

q=E/N=3.00×10−11J=187.266MeV.\boxed{q=E/N=3.00\times10^{-11}\,\mathrm J=187.266\,\mathrm{MeV}}.σqq=(.0018/.0600)2+(.04/2.00)2=.036056.\frac{\sigma_q}{q}=\sqrt{(.0018/.0600)^2+(.04/2.00)^2}=.036056.

(b) Interpretation and further calculation

σq=6.752MeV,q=(187.3±6.8)MeV.\boxed{\sigma_q=6.752\,\mathrm{MeV},\quad q=(187.3\pm6.8)\,\mathrm{MeV}}.z=187.266−1906.752=−.405consistent at this precision.\boxed{z=\frac{187.266-190}{6.752}=-.405}\quad\text{consistent at this precision}.

Physical check

Shared calibration errors would require a covariance term. A measurement of deposited energy need not equal the full nuclear Q value.