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NUC-01

Exponential decay

N = N0 e^{−λt}, A = λ N. Half-life T½ = ln2 / λ.

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DecayRutherford

Governing equation

N=N0eλt,T1/2=ln2/λN=N_0 e^{-\lambda t},\quad T_{1/2}=\ln 2/\lambda

where

N_0
Initial nuclei ()
\lambda
Decay constant (1/s)
t
Time (s)
N
Remaining ()
A
Activity (Bq)

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-01 — Exponential decay) is the form associated with Rutherford. Working symbols: N0N_0, λ\lambda, tt \rightarrow NN, AA. Each nucleus is memoryless. λ is a property of the species, not the sample size.

Purpose

Purpose: compute NN, AA from N0N_0, λ\lambda, tt in Nuclear physics via N=N0eλt,T1/2=ln2/λN=N_0 e^{-\lambda t},\quad T_{1/2}=\ln 2/\lambda N = N0 e^{−λt}, A = λ N. Half-life T½ = ln2 / λ. 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 N0=1.000e+6N_0 = 1.000e+6\,\mathrm{—}, λ=0.0101/s\lambda = 0.010\,\mathrm{1/s}, t=60.000st = 60.000\,\mathrm{s}, the governing relation N=N0eλt,T1/2=ln2/λN=N_0 e^{-\lambda t},\quad T_{1/2}=\ln 2/\lambda yields N=548811.64N = 548811.64\,\mathrm{—}, A=5488.12BqA = 5488.12\,\mathrm{Bq}. A decaying staircase of counts. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • Remaining N548811.64
  • Activity A5488.12 Bq
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NUC-01 · decay
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Narration of this film

A decaying staircase of counts.

Each nucleus is memoryless. λ is a property of the species, not the sample size.

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