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Light’s path to all these places in the body 47
Air Medium
Average distance between absorption events = 1/µa
Absorption
Intensity (depth) = initial intensity x e – µa x depth
exponential decay at a rate of µa
Mean free path
(i.e. average distance between ‘Micro’ scatter events)
= 1/µs
Scatter
Reduced mean free path
(i.e. average distance between ‘Macro’ scatter events at average anisotropy)
= 1/µs
Skin/
fur Soft tissue
Fat
Absorption Complex combination of
and scatter spread and decay Connective
tissue
Especially when we Bone
add all the dierent tissues
that make up anatomy into the picture
Figure 6.4 Pictorial representation of absorption, scatter, and the “real-life” combination of both. Illustrator: Elaine Leggett.
an ice pack, only the tissue underneath (or very close energy of the beam incident on a given spot PER UNIT
to) the ice pack is getting cold. But with laser, you will OF TIME and is measured in watts, with 1 watt = 1
be administering therapy well outside of where you see joule per second.
the light. I emphasize the word “incident” because we do not
This is a good thing, but also leads to some confusion. talk (in this industry) about the absorbed energy. In
There are two critical values: energy and power. fields that deal with X-rays, we do talk about absorbed
Energy is the total energy of the beam INCIDENT at a dose (in units of energy per volume or energy per mass
given spot and is measured in joules. Power is the total of tissue) because, for X-rays, absorption is the primary
Figure 6.5 (a, b) The effect of the angle of the incident beam on light dispersion.
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