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Understanding Neutron Radiography Post Exam Reading VIII-Part 2a of 2A

Understanding Neutron Radiography Post Exam Reading VIII-Part 2a of 2A

Understanding Neutron Radiography Post Exam Reading VIII-Part 2a of 2A

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The electron that is removed is then called a photoelectron. The incident<br />

photon is completely absorbed in the process. Hence it forms one <strong>of</strong> the<br />

reason for attenuation <strong>of</strong> X-ray beam as it passes through the matter.<br />

PEA is related to the atomic number <strong>of</strong> the attenuating medium (Z), the<br />

energy <strong>of</strong> the incident photon (E) and the physical density <strong>of</strong> the attenuating<br />

medium (ρ) by:<br />

PEA ∝ Z³ ·ρ / E³.<br />

Therefore, if Z doubles, PEA will increase by a factor <strong>of</strong> 8 (because 2³ is 8)<br />

and if E doubles, PEA will reduce by 8. As small changes in Z can have quite<br />

pr<strong>of</strong>ound changes in PEA this has practical implications in the field <strong>of</strong><br />

radiation protection and is why materials with a high Z such as lead (Z = 82)<br />

are useful shielding materials.<br />

Charlie Chong/ Fion Zhang<br />

http://radiopaedia.org/articles/photoelectric-effect

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