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NUC-12

Branching ratio

λ_i = b_i λ, A_i = b_i A. Partial width of one decay channel.

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DecayBranching

Governing equation

λi=biλ,Ai=biA\lambda_i=b_i\lambda,\quad A_i=b_i A

bi∈[0,1]b_i \in \left[0, 1\right]

where

A
Total activity (Bq)
b_i
Branching fraction (—)
A_i
Partial activity (Bq)

The figure, part by part

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NUC-12 · decay
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①

Governing law — red

λi=biλ,Ai=biA\lambda_i=b_i\lambda,\quad A_i=b_i A

bi∈[0,1]b_i \in \left[0, 1\right]

bi=0b_i = 0Ai=0A_i = 0

②

Domain of the variable — blue

b_i_{\min} = 0,\quad b_i_{\max} = 1

bi∈[0,1]b_i \in \left[0, 1\right]

bi=0b_i = 0bi=0b_i = 0

③

Response curve — green

λi=biλ,Ai=biA\lambda_i=b_i\lambda,\quad A_i=b_i A

bi∈[0,1]b_i \in \left[0, 1\right]

bi=0b_i = 0Ai=0A_i = 0

④

Rate of change — amber

dAidbi\frac{\mathrm{d}A_i}{\mathrm{d}b_i}

bi∈[0,1]b_i \in \left[0, 1\right]

bi=0.006b_i = 0.006Ai′=1×106A_i^{\prime} = 1\times 10^{6}

Lecture brief

Historical brief

Rutherford, Chadwick, the semi-empirical mass formula, fission (Hahn–Strassmann 1938) and fusion Q-values, then Compton and Bethe–Bloch stopping, are the nuclear toolkit. Decay, binding and dose start here. This sheet (NUC-12 — Branching ratio) is the form associated with Branching. Working symbols: AA, bib_i →\rightarrow AiA_i. Σ b_i = 1. Each channel is an independent Poisson process.

Purpose

Purpose: compute AiA_i from AA, bib_i in Nuclear physics via λi=biλ,Ai=biA\lambda_i=b_i\lambda,\quad A_i=b_i A λ_i = b_i λ, A_i = b_i A. Partial width of one decay channel. Use it when a real nuclear physics question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given A=1.000e+6 BqA = 1.000e+6\,\mathrm{Bq}, bi=0.350 —b_i = 0.350\,\mathrm{—}, the governing relation λi=biλ,Ai=biA\lambda_i=b_i\lambda,\quad A_i=b_i A yields Ai=350000.00 BqA_i = 350000.00\,\mathrm{Bq}. A fork of two decay arrows. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • Partial activity A_i350000.00 Bq
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NUC-12 · decay
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Narration of this film

A fork of two decay arrows.

Σ b_i = 1. Each channel is an independent Poisson process.

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