Experimental results
Experiments were done on different thicknesses of human dermis.
The first set consists of nine measurements on five different
samples ranging 200-400 m thick. The second set used 24
samples (including twelve 20 m samples) on thin microtomed
sections varying from 20-100 m thick. The attenuation coefficient
was obtained by making total attenuation measurements
on all samples and averaging the results. The total attenuation
measurement so obtained is 190cm-1 and was used to convert all
sample thicknesses into optical depths. These optical depths
were used to calculate the correction factors. A typical fit
is shown in Figure 5.10.
Figure 5.10:
Experimental data and fitted phase function for
100 m thick human dermis. Solid line is the fitted phase
function. Squares and error bars indicate measured values and
uncertainty in measurements.
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Figure:
The measured anisotropy factor
for human dermis
as a function of sample thickness. The solid line indicates
the dependence of the measurement technique on sample thickness.
The limiting value of
is 0.92. Error bars indicate the
standard deviation of the data.
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Figure 5.12:
The measured isotropy factor
for human dermis
as a function of sample thickness. The limiting value of
is
0.05. Error bars indicate the standard deviation of the data.
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The Henyey-Greenstein phase function parameter
gHG as a function
of thickness is shown in Figure 5.11. The limiting value for
the anisotropy factor was
gHG=0.92. The error bars are the standard
deviation of the fitted values of
gHG for each sample thickness.
The increased error for the thinnest samples
is caused
by tearing occurring during the tissue preparation process.
The solid curve is identical to that in Figure 5.7 and is included
to indicate the dependence of the fitted value of
gHG on the
thickness of the sample. Figure 5.12 shows corrected values
for the isotropy
as a function of thickness.
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