Photon Therapy: The Basics

 

The Inverse Square Law:

 

image001

  

    1. Undoubtedly one of the most useful properties of radiation emitted from a point source is the inverse square relationship which states that the radiation fluence falls off at a rate proportional to image002 where r is the distance from the point source.

    2. Any radiation diverging from a point in free space exhibits this phenomenon.  However, in the real world radiation does not always follow this relationship due to the following:

      1. attenuation,

      2. scattering, and

      3. discrete sources which are not a point.

        1. If you are far enough away from a discrete source it will still approximately act like a point source usually 2X the longest dimension would be appropriate.

    3. The way you utilize this effect in practice is as follows

      1. Suppose you measure some amount of radiation X at a distance of 100 cm.

      2. How much radiation would you measure with the same detector at 110 cm?

      3. This would be equal to: image004.

 

Scattering Angle and Energy:

 

image006

 

    1. For low energy photons (30-50 kV) undergoing Compton scattering, they are almost as likely to be scattered backward as they are to be forward scattered.

    2. However, as the energy of the photons increases, it becomes less and less likely that they will change direction as abruptly (consider it inertia), and in the megavoltage energy range, almost all scattering occurs in a forward direction with very little side-scattering or backscattering.

    3. This is true for electrons as well and is partially responsible for the changes in dmax and surface dose seen below.

 

Attenuation Coefficients:

 

    1. There are three different attenuation coefficients that are useful in describing photon interactions in a medium:

      1. Mass attenuation coefficient image007 which is used to describe attenuation: how many photons are removed per unit distance normalized to the medium's density (units of cm2/g).

      2. Mass energy transfer coefficient image009 which is used to describe the amount of energy released per unit path length in a medium normalized to the density of the medium.

        1. This is related to KERMA image011 where image013 is the photon energy fluence.

      3. Mass energy absorption coefficient image015 which is used to describe the amount of energy absorbed in a medium per unit path length normalized to the density of the medium.

        1. This is related to the Dose (D) by: image017 where image013 is the photon energy fluence.

 

Anonymous
2014-06-25, 16:14
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Thanks so much for providing this resource!