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link to lecture transcript - UT-H GSBS Medical Physics Class Site

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What about the scatter coefficient? Remember when we have attenuation, two<br />

things can happen. Some of the energy can be transferred <strong>to</strong> charged particles,<br />

while some of the energy can go <strong>to</strong> a scattered pho<strong>to</strong>n. So the scatter coefficient is<br />

going <strong>to</strong> be equal <strong>to</strong> the <strong>to</strong>tal coefficient minus the energy transfer coefficient.<br />

At low energies, the energy transfer is small, so the scatter coefficient is<br />

approximately equal <strong>to</strong> the <strong>to</strong>tal attenuation coefficient. Comp<strong>to</strong>n scatter is not a<br />

good process for transferring energy <strong>to</strong> charged particles at low energies, but this is<br />

also consistent with classical scatter, so we do wind-up getting the coherent scatter<br />

in the limit of low energies.<br />

At high energies, almost all of the energy gets transferred <strong>to</strong> charged particles.<br />

Consequently, q y the scatter coefficient approaches pp zero. So the scatter coefficient<br />

goes between the <strong>to</strong>tal attenuation coefficient at low energies and zero at high<br />

energies.<br />

Now, let’s use this information about coefficients <strong>to</strong> deduce some properties of<br />

energy transfer and energy absorption.<br />

17

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