Biomedical Engineering Reference
In-Depth Information
Fig. 8.23 Identification of target cumulative APSD for CFC suspension MDI w9j601 : fit of logis-
tic model to cumulative mass-weighted APSD; %LC % label claim; “APS” in equation = aerody-
namic particle size (μm)
MMAD value, and its pseudo R 2 values were computed as a function of the displaced
MMAD . Limits in terms of MMAD were then established by selecting arbitrary R 2
values (0.9, 0.8, 0.7, and 0.6) and selecting the corresponding MMAD values as the
assumed limits. The calculation for the pseudo R 2 is given by Eq. (8.5) for clarity.
n
n
å
å
2
2
(
yy
-
)
(%
LC
-
%
LC
)
i
i
Displaced
Reference
2
i
=
1
i
=
1
R
=
=
(8.5)
n
n
å
å
(
yy
-
)
2
(%
LC
-
%
LC
)
2
Displaced
i
i
Displaced
i
=
1
i
=
1
It is important to note that the differences were calculated for particular fixed
particle sizes as measures of distance between the curves vertically. This is one
approach for determining a bound around the target/reference APSD curve that
defines a range of acceptable MMAD values.
Again the reader is reminded that these selections are not connected in any man-
ner to the actual quality limits for the studied products. They were selected exclu-
sively to study the characteristic of the APSD-related metrics. Figure 8.24 illustrates
this process for OIP w9j601 when R 2 is set at 0.9. The entire set of limits (Table 8.6 )
employed for constructing OCCs were obtained via this process.
Using these assumed limits for the MMAD values, both cumulative APSDs
(Fig. 8.25 ) and APSDs plotted in the form of individual values of API per stage
(Fig. 8.26 ) could be constructed for hypothetical APSDs at the assumed limits. Note
that this exercise considers the case of a shift in MMAD of the distribution without
a change in its shape.
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