Dimensional quantities
Tissue is assumed to be a random turbid medium, with variations in the
optical properties small enough to prevent localized absorption. In other words,
tissue is considered to have volumetric scattering and absorption properties
rather than being composed of discrete scattering and absorption centers
distributed in a non-scattering, non-absorbing medium. The advantage to the
distributed scattering center approach is that for perfect spheres the phase
function is known, however there is little similarity between perfect spheres and
tissue. Volumetric absorption (or scattering) is obtained by multiplying an
absorption (or scattering) cross section with the density of absorbers (or
scatterers) [31]. This is how the absorption coefficients
and
scattering coefficient
are defined. The scattering and absorption coefficient
are typically measured in inverse millimeters and the reciprocal of these
coefficients is the average distance that light will travel before being scattered or
absorbed, respectively.
The thickness of the slab is denoted by d. In addition to the thickness,
light propagation through a slab is determined by three parameters: the
absorption and scattering coefficients and the phase function. The phase function
is the fraction of light scattered into the direction of the unit vector
by light
incident from the direction of the unit vector
.
The phase function is discussed in
detail below.
The radiance is
;
the position is denoted by the vector r and the
radiance is specified by the direction of the unit vector
.
The radiance has units
of energy per area per solid angle (Watts sr-1 cm2). Sometimes this is called
``specific intensity'' or just ``intensity.''
The fluence
is the total radiance at a point r. The fluence is obtained
by integrating the radiance over all angles. The product of the fluence and the
absorption coefficient equals the heat source: the amount of energy deposited in
a unit volume of tissue.
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