By Marco Zaider, Harald H. Rossi

We have thought of it to be a tough task to supply a whole exposition facing the character of radiation, its results, and security opposed to it to staff in health-related actions. "Radiation" (and extra accurately "ionizing radiation") is emitted by means of X-ray machines, nuclear reactors, and nuclear guns, but additionally comes from normal assets to which we're all uncovered. it'll were more uncomplicated to accommodate this topic sector with the terminology and arithmetic hired by way of experts. besides the fact that, even supposing lots of the capability readers most likely have got extra pertinent wisdom, we think not more than a highschool schooling in technology and arithmetic and the problem used to be to supply greatest info inside of this constraint. This publication comprises 5 sections: (A) Radiation Physics, (B) Radiological Physics, (C) Radiation Biology, (D) Radiation results on Human Populations, and (E) Radiation defense. every one part is preceded by means of a synopsis protecting its crucial gains. It offers enough details to let readers to acquire a basic below­ status of the topic of the part and an enough heritage for comprehension of different sections. The extra exact presentation within the bulk of every part is via appendixes that more often than not include extra complex subject matters. This scheme unavoidably comprises a few repetition yet allows a extra versatile technique for readers who're in particular drawn to the contents of specific sections.

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X Figure 7. Penetration of neutrons through a slab of thickness LiN _ cr(SLix)p _ A N S - crtlXP /';x. (19) An equivalent fonn of Eq. (9) is: (20) where is the neutron fluence (n/m 2) and nt is the total number of target nuclei in the absorber. A statement regarding cr must at a minimum include the nature of the radiation, the target, and the type of interaction. , the cross section for 90° scattering of 100-keV electrons by hydrogen). It is convenient to consider interactions of uncharged particles separately from those of charged particles, not only because the fonner give rise to the latter but also because of the frequency of interaction.

A typical reactor generates some 106 kW of electrical power. The core of a reactor is intensely radioactive and must be surrounded by massive shielding (usually made of concrete). Frequently the reactor is provided with a secondary radiation shield, often in the form of a containment shell (a hemispherical structure made of steel and concrete surrounding the entire reactor). The main role of the containment shell is to prevent the escape into the atmosphere of radioactive fission byproducts that would be released in the event of a core meltdown or any other accident.

It is convenient to consider interactions of uncharged particles separately from those of charged particles, not only because the fonner give rise to the latter but also because of the frequency of interaction. Uncharged particles (photons and neutrons) generally lose a substantial fraction of their energy in each of relatively few interaction before they are absorbed. On the other hand, a 5-MeV a. particle undergoes more than 50,000 collisions before it is stopped. Photons At the energies of concern here «50 MeV) there are three main processes by which photons interact with matter: the photoelectric effect, Compton scattering, and pair production (Fig-Me 8).

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