DISTRIBUTION WIDTHS
Most instruments are used to measure the particle size distribution, implying an
interest in the width or breadth of the distribution. Experienced scientists typically
shun using a single number answer to the question “What size are those particles?”,
and prefer to include a way to define the width. The field of statistics provides
several calculations to describe the width of distributions, and these calculations
are sometimes used in the field of particle characterization. The most common
calculations are standard deviation and variance. The standard deviation (St Dev.)
is the preferred value in our field of study. As shown in Figure 4, 68.27% of the total
population lies within +/- 1 St Dev, and 95.45% lies within +/- 2 St Dev.
Although occasionally cited, the use of standard deviation declined when hardware
and software advanced beyond assuming normal or Rosin-Rammler distributions.
Once “model independent” algorithms were introduced many particle scientists
began using different calculations to describe distribution width. One of the common
values used for laser diffraction results is the span, with the strict definition shown in
the equation below (2):
In rare situations the span equation may be defined using other values such as
Dv0.8 and Dv0.2. Laser diffraction instruments should allow users this flexibility.
An additional approach to describing distribution width is to normalize the standard
deviation through division by the mean. This is the Coefficient of Variation (COV)
(although it may also be referred to as the relative standard deviation, or RSD).
Although included in HORIBA laser diffraction software this value is seldom used as
often as it should given its stature. The COV calculation is both used and encouraged
as a calculation to express measurement result reproducibility. ISO13320 (ref. 4)
encourages all users to measure any sample at least 3 times, calculate the mean, st
dev, and COV (st dev/mean), and the standard sets pass/fail criteria based on the
COV values.
figure 4
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