| Item | Key Features | Notes / Differences |
|---|---|---|
| Photon (X-ray, gamma) | Electromagnetic, low LET (~0.2–3 keV/μm) | Widely used in diagnostics and radiotherapy |
| Electrons | Charged particles, moderate LET (~0.2–2 keV/μm) | Used in superficial treatments |
| Protons | Heavy charged particle, high LET (~10–100 keV/μm) | Targeted therapy, Bragg peak effect |
| Alpha particles | He nucleus, high LET (~100 keV/μm), heavily ionizing | Limited penetration, high damaging capacity |
| Neutrons | Neutral; indirect ionization via nuclear reactions | Significant biological effectiveness, hard to shield |
Ionizing Radiation
├─ Electromagnetic Radiation
│ ├─ X-rays
│ └─ Gamma rays
├─ Particulate Radiation
│ ├─ Electrons
│ ├─ Protons
│ ├─ Alpha particles
│ └─ Neutrons
└─ Biological Target
├─ DNA & Cellular Structures
└─ Water & free radicals
Pon a prueba tus conocimientos sobre Fundamentals of Ionizing Radiation in Medicine con 10 preguntas de opción múltiple con correcciones detalladas.
1. Who discovered X-rays and in which year?
2. What is the primary purpose of the 'activity' (A) measurement in ionizing radiation?
Memoriza los conceptos clave de Fundamentals of Ionizing Radiation in Medicine con 10 tarjetas de memoria interactivas.
What is ionizing radiation?
Ionizing radiation has enough energy to create ion pairs by ejecting electrons from atoms or molecules. It includes electromagnetic types like X-rays and gamma rays, as well as particles such as electrons, protons, alphas, and neutrons.
Ionizing radiation — definition?
Energy capable of ionizing atoms or molecules.
Name and briefly describe the three main photon interaction mechanisms relevant in medical physics.
The photoelectric effect involves photon absorption where an inner-shell electron is ejected, dominant at low energies with high atomic number materials. Compton scattering is when photons scatter off electrons, transferring part of their energy, important at intermediate energies (~4-25 MeV). Pair production occurs when a photon with energy above 1.022 MeV converts into an electron-positron pair near a nucleus, relevant at energies >10 MeV.
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