Phantoms with controlled optical properties are often used for calibration and standardization. The phantoms
are typically prepared by adding absorbers and scatterers to a clear host material. It is usually assumed that the
scatterers and absorbers are uniformly dispersed within the medium. To explore the effects of this assumption, we
prepared paired sets of polyurethane phantoms (both with identical masses of absorber, India ink and scatterer,
titanium dioxide). Polyurethane phantoms were made by mixing two polyurethane parts (a and b) together
and letting them cure in a polypropylene container. The mixture was degassed before curing to ensure a
sample without bubbles. The optical properties were controlled by mixing titanium dioxide or India ink into
polyurethane part (a or b) before blending the parts together. By changing the mixing sequence, we could
change the aggregation of the scattering and absorbing particles. Each set had one sample with homogeneously
dispersed scatterers and absorbers, and a second sample with slightly aggregated scatterers or absorbers. We
found that the measured transmittance could easily vary by a factor of twenty. The estimated optical properties
(using the inverse adding-doubling method) indicate that when aggregation is present, the optical properties are
no longer proportional to the concentrations of absorbers or scatterers.
The main objective of this study was to construct a double integrating sphere system and to verify its performance using
Intralipid fat emulsion. The final goal was to be able to determine optical properties of various turbid suspensions with
the proposed system. Online measurements even would have been possible as backscattering and forward scattering were
measured simultaneously. The measured suspension was injected in a cuvette placed between two integrating spheres
and illuminated with a laser through the first sphere. The diameter of the spheres was 8" and the diameter of the sample
port could have been varied up to 2.5". The cuvette was made of plastic and optical grade glass and its diameter was
sufficient to cover the sample port area. The sample thickness in the measurement cuvette was 5 mm. Optical powers
were detected using fiber coupled photodiodes. There was one diode for each sphere and one for the unscattered light at
the opposite end of the sphere system facing towards the laser. The measured optical powers were converted to
absorption coefficient, scattering coefficient and if possible to anisotropy using an inverse adding-doubling method. The
results measured for the Intralipid using the described system corresponded with those documented in published
literature. A number of pulp samples with unknown optical properties were measured with encouraging results.
However, the differences between different pulps and fillers are so small that, in the future, the focus will be in error
source elimination to achieve reasonable accuracy.
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