Physica

00 Foundations

Branching ratio and partial activity

Partial emission rate A_i = A × BR_i × n_i for photons, β or α of a given branch.

Listen

Listen · English

Simulation

Branching ratio and partial activity — Change the numbers; the scene follows.

Where it works

Hot lab

Hot lab

Dose calibrator

In the dose calibrator well — assayed activity, decay between two times, Marinelli.

Open this machine

Formula

Ai=ABRini,ΓairiBRiEiA_i = A\cdot BR_i\cdot n_i,\quad \Gamma_{\mathrm{air}}\propto \sum_i BR_i E_i

Typical values

Variables

Results

  • A_i

    Partial activity

    325.6MBq

  • Emission rate

    3.256e+8s⁻¹

Explanation

Ai=ABRini,ΓairiBRiEiA_i = A\cdot BR_i\cdot n_i,\quad \Gamma_{\mathrm{air}}\propto \sum_i BR_i E_i

What it means

Almost no radionuclide emits a single radiation. ⁹⁹ᵐTc: 88% 140 keV γ (the imaging photon), internal conversion and a few other lines. ¹⁸F: 97% β⁺ (hence 194% of 511 keV annihilation photons per decay) and 3% EC. Dose constants, gamma constants and imaging yields always fold in the branching ratio. This is a working relation in Radiation physics.

Where it is used

Clinically it sits on the Hot lab — Dose calibrator. In the dose calibrator well — assayed activity, decay between two times, Marinelli. Radiation physics lives at the x-ray target, the linac head, and inside the patient: how a photon is born, how it scatters, and how it dies. Use these relations before you trust a spectrum, a wall, or a kV-versus-MV contrast argument.

Hot lab · Open this machine

How to use it

Enter total activity, branching ratio (0–1) and emissions per decay n (2 for annihilation). Read the partial activity and the photon emission rate. For PET n=2 and BR=β⁺ fraction. Change one input and watch the curve and the simulation follow.

Symbols

  • ATotal activity370 MBq
  • BRBranching ratio0.88
  • nEmissions per decay1

Worked example

A typical case from the default values: A = 370 MBq (Total activity); BR = 0.88 (Branching ratio); n = 1 (Emissions per decay). Substituting into the relation gives A_i = 325.6 MBq; ṅ = 3.256e+8 s⁻¹. These are teaching numbers — align them with your machine.

Typical values give

  • A_i = 325.6MBq
  • = 3.256e+8s⁻¹

Where it comes from

The displayed formula is the working relation. Partial emission rate A_i = A × BR_i × n_i for photons, β or α of a given branch. Usual reference: ICRP 107 / Cherry. Derive it in the specialty lesson, then return here to pin the numbers.

Reference: ICRP 107 / Cherry

Assumptions & limits

Single line. Does not build a full decay scheme, nor include internal-conversion electrons or x-ray fluorescence that follow EC/IT.

Pitfalls

Do not mix free-electron Compton kinematics with photoelectric-dominated kV imaging. Check keV versus MeV, and never treat a spectrum as one photon. Single line. Does not build a full decay scheme, nor include internal-conversion electrons or x-ray fluorescence that follow EC/IT.

Keep this

Photons do not deposit dose; the electrons they set in motion do. Single line. Does not build a full decay scheme, nor include internal-conversion electrons or x-ray fluorescence that follow EC/IT.

In this specialty

Radiation physics