2015 AIChE Annual Meeting Proceedings
(410g) Analysis of Transient Permeation and Conduction in Composites with External Transport Resistance
Authors
Laplace transform methods are known to provide ?Early-Time? series
solutions (with fewer significant terms as t®0)
to linear partial differential equations governing transient permeation
and heat conduction. These solutions tend to be particularly convenient
because, unlike some ?Long-Time? solutions, Early-Time solutions do not involve
eigenvalues defined by transcendental equations.
The Early-Time approach is applied here to the analysis of
permeation in two-layer composite membranes with external mass transfer
resistance. The governing equations are then :
subject to:
The goal is an expression for M(t), the time course of the cumulative
mass permeated per unit area, i.e.:
or, in dimensionless terms:
Notably, Sakai (1922) derived a
?Long-Time? series solution to Eqs. 1 in the general case of an arbitrary
number of layers, but with negligible external mass transfer resistance.
For purposes of deriving the Early-Time solution, Laplace-transform
operator is
defined as usual by:
Eqs. 1 are thereby transformed to easily solved ordinary
differential equations. The end result is the following expression for the
transform of m:
Recovery of and,
in turn, requires
inverse transformation of Eq. 5. ScientistR numerical inversion software
(Micromath Inc.) provides essentially exact results with which those based on truncated
Early-Time(?ET?) series will be compared.
The latter series emerge from inverse transformation of the
expression to which simplifies
when s is large. When only the lead terms are retained, the result is:
Retaining additional terms extends the time over which the Early-Time
solution is accurate. In many cases of practical interest, only the lead terms
are necessary to accurately model essentially the entire non-steady-state
region.
Sakai, S. (1922) ?Linear conduction of heat through a series
of connected rods,? Sci. Rep. Tohoku Imperial Univ., Ser. I (Math, Phys.,
Chem.), 11, 351- 378.