Nuclear Fission: The Basic Process — Question 6

Section 43-1 · Physics pages 7162–7163

Question 6 Prompt and delayed energy create different calorimeter readings A burst of 1012 fissions deposits 180 MeV promptly per event and an additional 12 MeV per event through a single exponential delayed component with mean time τ = 30.0 s. Ignore neutrino energy; all stated energy is absorbed. Use 1 MeV = 1.602 × 10−13 J. t E(t) Schematic; labels, not drawing lengths, specify the data. (a) Derive total absorbed energy E(t) for t after the prompt pulse. (b) Find E at 30 s and the delayed thermal power at that time.
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Question 6 - Solution Prompt and delayed energy create different calorimeter readings t E(t) (a) Method and calculation E(t) = N{Ep + Ed[1 −e−t/τ]} ⇒E(t) = 28.836 + 1.9224(1 −e−t/30) J . E(0+) = 28.836 J, E(∞) = 30.7584 J. (b) Interpretation and further calculation E(30) = 30.0512 J . Pd = NEd τ e−t/τ ⇒Pd(30) = .023574 W . Physical check The delayed power is the derivative of only the delayed energy. A short observation window underestimates the eventual calorimetric yield.

Question 6

Prompt and delayed energy create different calorimeter readings

A burst of 101210^{12} fissions deposits 180 MeV promptly per event and an additional 12 MeV per event through a single exponential delayed component with mean time τ=30.0\tau=30.0 s. Ignore neutrino energy; all stated energy is absorbed. Use 1MeV=1.602×10−131\,\mathrm{MeV}=1.602\times10^{-13} J.

Diagram shown in the original SVG worksheet.

  1. Derive total absorbed energy E(t) for t after the prompt pulse.

  2. Find E at 30 s and the delayed thermal power at that time.

Question 6 - Solution

Prompt and delayed energy create different calorimeter readings

Diagram shown in the original SVG worksheet.

(a) Method and calculation

E(t)=N{Ep+Ed[1−e−t/τ]}⇒E(t)=28.836+1.9224(1−e−t/30)J.E(t)=N\{E_p+E_d[1-e^{-t/\tau}]\}\Rightarrow\boxed{E(t)=28.836+1.9224(1-e^{-t/30})\,\mathrm J}.E(0+)=28.836J,E(∞)=30.7584J.E(0^+)=28.836\,\mathrm J,\qquad E(\infty)=30.7584\,\mathrm J.

(b) Interpretation and further calculation

E(30)=30.0512J.\boxed{E(30)=30.0512\,\mathrm J}.Pd=NEdτe−t/τ⇒Pd(30)=.023574W.P_d=\frac{NE_d}{\tau}e^{-t/\tau}\Rightarrow\boxed{P_d(30)=.023574\,\mathrm W}.

Physical check

The delayed power is the derivative of only the delayed energy. A short observation window underestimates the eventual calorimetric yield.