Author:
PHILLIPS C. G.,KAYE S. R.
Abstract
We consider the transport of a tracer substance in Poiseuille flow
through a pipe
lined with a thin, fixed wall layer in which the tracer is soluble. A formal
solution
is given for the variation of concentration with time at a fixed downstream
position
following an initial release of tracer. Asymptotic approximations are derived
assuming
that: (i) the Péclet number is large; (ii) the time scale for diffusion
across the wall
layer is much larger than that for diffusion across the fluid phase and
(iii) the
dimensionless distance downstream of the point of release, z,
is large. This means that
the transverse concentration variation is small within the fluid phase,
so that transport
is dominated by the exchange of tracer between the phases and radial diffusion
within
the wall layer. The character of the concentration transient is found to
be determined
by two dimensionless numbers, an absorption parameter κ and an effective
wall
layer thickness ν (both rescaled to take account of the ratio of diffusivities
in the two
phases); by assumption (ii), ν is large. Several different regimes are
possible, according
to the values of κ, ν and z. At sufficiently
large distances, a Gaussian approximation,
analogous to Taylor's solution, is applicable. At intermediate distances,
provided
κ is not too large, a highly skewed transient is predicted.
If κ is small, there exists
another region further upstream where the effect of the wall is negligible,
and Taylor's
Gaussian approximation applies. More complicated behaviour occurs in the
zones
of transition between these three regions. The behaviour described is expected
to be
typical of a range of similar systems. In particular, it may be shown that
the basic
form of the skewed approximation is insensitive to the geometry of the
system, and
also applies when the Péclet number is of order unity.
Publisher
Cambridge University Press (CUP)
Subject
Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics
Cited by
22 articles.
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