ISO 24427:2025
(Main)Radiological protection — Medical proton accelerators — Requirements and recommendations for shielding design and evaluation
Radiological protection — Medical proton accelerators — Requirements and recommendations for shielding design and evaluation
This document is applicable to the radiation shielding design and evaluation work for medical proton accelerators of proton energies ranging from 70 MeV to 250 MeV, with subsystems such as beam transport system and nozzle components. The radiation protection recommendations given in this document cover the aspects relating to regulations, shielding design goals and other design criteria, role of the manufacturers, of the radiation protection officer or qualified expert, the medical physicist, the licensee and interactions between them, sources and radiations around a proton accelerator, shielding for accelerators and its subsystems (including shielding materials and transmission values, calculations for various room configurations, duct impact on radiation protection) and the radiological measurements. FLASH proton therapy is not covered by this document. NOTE 1 Annex A provides a list of the most used Monte-Carlo codes for shielding calculation. NOTE 2 Annex B provides the analytical methods and the corresponding necessary data for shielding calculation. NOTE 3 Annex C provides a set of examples on shielding calculation of barriers, maze and skyshine problems. NOTE 4 Annex D provides radiation shielding consideration on special topics.
Radioprotection — Accélérateurs médicaux de protons — Exigences et recommendations pour la conception et l'évaluation du blindage
General Information
Standards Content (Sample)
International
Standard
ISO 24427
First edition
Radiological protection —
2025-09
Medical proton accelerators
— Requirements and
recommendations for shielding
design and evaluation
Radioprotection — Accélérateurs médicaux de protons —
Exigences et recommendations pour la conception et l'évaluation
du blindage
Reference number
© ISO 2025
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ii
Contents Page
Foreword .iv
Introduction .v
1 Scope . 1
2 Normative references . 1
3 Terms and definitions . 1
3.1 Quantities .2
3.2 Definitions other than quantities .4
4 Shielding design goals and other design criteria . 6
4.1 Shielding design goals .6
4.2 Shielding design assumptions and conditions .7
5 Role of stakeholders and the interactions . 7
5.1 General .7
5.2 Manufacturer of the proton therapy system .8
5.3 General contractor/architectural firm .8
5.4 Radiation safety officer or other .9
5.5 The medical physicist or other .9
5.6 The licensee or other .10
6 Radiation sources of a medical proton accelerator . 10
6.1 General .10
6.2 Prompt radiation sources .10
6.2.1 Secondary neutron .10
6.2.2 Photon radiation .10
6.3 Radiation during shut down .10
7 Shielding materials and transmission . .11
7.1 General .11
7.2 Shielding materials .11
7.3 Transmission .11
8 General formalism .12
9 Shielding calculation . 14
9.1 General .14
9.2 Monte-Carlo simulation .14
9.2.1 General .14
9.2.2 Basic requirement on Monte-Carlo simulation . 15
9.3 Analytical methods . 15
9.3.1 Shielding barrier. 15
9.3.2 Mazes .16
9.3.3 Skyshine .16
9.3.4 Duct .17
10 Shielding evaluation. 17
10.1 General .17
10.2 Measuring equipment and methodology .17
10.3 Evaluation .18
Annex A (informative) Monte-Carlo simulation for the radiation shielding of medical proton
accelerators . 19
Annex B (informative) Analytical methods for the radiation shielding of medical proton
accelerators .22
Annex C (informative) Examples of radiation shielding calculation .31
Annex D (informative) Special topics .44
iii
Foreword
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iv
Introduction
Protons deliver most of their energy at a prescribed, programmable distance inside the body, known as the
Bragg Peak. With this feature, proton therapy is used to treat many cancers and is particularly appropriate in
situations where treatment options are limited and conventional radiotherapy using photon beam presents
unacceptable risks to patients. The use of proton accelerators to administer external beam radiation has
been evolving and the proton therapy centres are rising worldwide.
A typical large proton therapy centre consists of an injector, a cyclotron or synchrotron to accelerate the
particles, high-energy beam selection and transport system, several treatment rooms (fixed beam and/or
gantry) and, occasionally, a research room. Strong secondary radiation, particularly high energy neutrons,
is produced at locations where beam losses occur. Such losses may occur in the cyclotron or synchrotron
along the beam transport system during acceleration, extraction, energy degradation and transport of the
protons to the treatment room, and in the treatment and research nozzles. In addition, the production of
proton beam interactions in the patient, beam stop, or dosimetry phantom also results in stray radiation
production. As a result, meters-thick barriers are generally used around the entire accelerator system.
The rad
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