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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