WHEN TO CHOOSE DYNAMIC LIGHT SCATTERING
Dynamic Light Scattering (DLS) can measure suspensions and emulsions from
1nm to 1µm. Both the lower and upper limits are sample dependent. The
lower limit is influenced by concentration and how strongly
the particles scatter
light. A low concentration sample of weakly scattering particles near 1nm can
be extremely difficult or at least difficult to reproduce. The upper size limit is
determined mainly by the density of the particles. DLS algorithms are based on
all particle movement coming from Brownian motion. Motion due to settling is not
interpreted correctly by DLS systems.
In addition, particles settled on the bottom
of the sample cuvette can not be inspected by the laser light source. Particles
with a high density will settle more quickly than low density particles. The upper
limit of DLS may be 8µm for emulsion samples where the two phases have
similar density. The upper limit of uranium particles may be as small as 300nm.
The upper limit of particles with a density of 1.7 may be around 1µm.
Using DLS does not require any knowledge of the sample RI (it would
be required
to convert from intensity to volume distribution), or concentration. What is
required is viscosity, especially for higher concentration samples. Although most
modern DLS systems claim the ability to work at higher concentrations, this
is again sample dependent. Serious DLS work could
involve a dilution study
to determine the nature of the particle-particle interactions and presence of
multiple scattering. Easy samples are simply a matter of pipetting the sample
into a cuvette and clicking one button. More sophisticated DLS systems can also
measure other sample characteristics including zeta potential, molecular weight,
and second virial coefficient. Generating this additional
information may require a
greater skill set of the operator.
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